From 6730974c904b3bce13c8457bb94d066a8bceca38 Mon Sep 17 00:00:00 2001 From: giozu Date: Mon, 26 Aug 2024 18:43:11 +0200 Subject: [PATCH 01/15] header update --- include/MainVariables.h | 2 +- include/Sciantix.h | 2 +- include/classes/Gas.h | 2 +- include/classes/InputVariable.h | 2 +- include/classes/Material.h | 2 +- include/classes/Matrix.h | 2 +- include/classes/Model.h | 2 +- include/classes/SciantixArray.h | 2 +- include/classes/SciantixVariable.h | 2 +- include/classes/Simulation.h | 2 +- include/classes/Solver.h | 2 +- include/classes/System.h | 2 +- include/classes/Variable.h | 2 +- include/file_manager/Initialization.h | 2 +- include/file_manager/InputInterpolation.h | 2 +- include/file_manager/InputReading.h | 2 +- include/file_manager/TimeStepCalculation.h | 2 +- include/models/GasDiffusion.h | 2 +- include/models/StoichiometryDeviation.h | 2 +- include/namespaces/Constants.h | 2 +- include/namespaces/ErrorMessages.h | 2 +- include/operations/SetGas.h | 2 +- include/operations/SetMatrix.h | 2 +- include/operations/SetSystem.h | 2 +- include/operations/SetVariables.h | 2 +- include/operations/SetVariablesFunctions.h | 2 +- src/MainSCIANTIX.C | 2 +- src/MainVariables.C | 2 +- src/Sciantix.C | 2 +- src/classes/Matrix.C | 2 +- src/classes/SciantixVariable.C | 2 +- src/classes/Simulation.C | 2 +- src/classes/Solver.C | 2 +- src/classes/System.C | 2 +- src/file_manager/Initialization.C | 2 +- src/file_manager/InputInterpolation.C | 2 +- src/file_manager/InputReading.C | 2 +- src/file_manager/Output.C | 2 +- src/file_manager/TimeStepCalculation.C | 2 +- src/models/Burnup.C | 2 +- src/models/EffectiveBurnup.C | 2 +- src/models/GapPartialPressure.C | 2 +- src/models/GasDecay.C | 2 +- src/models/GasDiffusion.C | 2 +- src/models/GasProduction.C | 2 +- src/models/GrainBoundaryMicroCracking.C | 2 +- src/models/GrainBoundarySweeping.C | 2 +- src/models/GrainBoundaryVenting.C | 2 +- src/models/GrainGrowth.C | 2 +- src/models/HighBurnupStructureFormation.C | 2 +- src/models/HighBurnupStructurePorosity.C | 2 +- src/models/InterGranularBubbleBehavior.C | 2 +- src/models/IntraGranularBubbleBehaviour.C | 2 +- src/models/StoichiometryDeviation.C | 2 +- src/models/UO2Thermochemistry.C | 2 +- src/namespaces/ErrorMessages.C | 2 +- src/operations/SetGas.C | 2 +- src/operations/SetMatrix.C | 2 +- src/operations/SetSystem.C | 2 +- src/operations/SetVariables.C | 2 +- src/operations/UpdateVariables.C | 2 +- 61 files changed, 61 insertions(+), 61 deletions(-) diff --git a/include/MainVariables.h b/include/MainVariables.h index 70b26332..697c8150 100644 --- a/include/MainVariables.h +++ b/include/MainVariables.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/Sciantix.h b/include/Sciantix.h index c1cf5757..e7ab520e 100644 --- a/include/Sciantix.h +++ b/include/Sciantix.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/Gas.h b/include/classes/Gas.h index 5f3da015..d051bfc6 100644 --- a/include/classes/Gas.h +++ b/include/classes/Gas.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/InputVariable.h b/include/classes/InputVariable.h index 68714c64..b00bd9c1 100644 --- a/include/classes/InputVariable.h +++ b/include/classes/InputVariable.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/Material.h b/include/classes/Material.h index 3d4e67d6..74b07e7b 100644 --- a/include/classes/Material.h +++ b/include/classes/Material.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/Matrix.h b/include/classes/Matrix.h index e312e829..1601c7b7 100644 --- a/include/classes/Matrix.h +++ b/include/classes/Matrix.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/Model.h b/include/classes/Model.h index aea85e9f..5cd9678d 100644 --- a/include/classes/Model.h +++ b/include/classes/Model.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/SciantixArray.h b/include/classes/SciantixArray.h index 2124894d..36a15e5a 100644 --- a/include/classes/SciantixArray.h +++ b/include/classes/SciantixArray.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/SciantixVariable.h b/include/classes/SciantixVariable.h index 0ff62500..89f64a8a 100644 --- a/include/classes/SciantixVariable.h +++ b/include/classes/SciantixVariable.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/Simulation.h b/include/classes/Simulation.h index b856d5ff..f3aff192 100644 --- a/include/classes/Simulation.h +++ b/include/classes/Simulation.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/Solver.h b/include/classes/Solver.h index 49aa2a41..82919be1 100644 --- a/include/classes/Solver.h +++ b/include/classes/Solver.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/System.h b/include/classes/System.h index 66fb46c7..2e4fbe00 100644 --- a/include/classes/System.h +++ b/include/classes/System.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/classes/Variable.h b/include/classes/Variable.h index 97069600..69fae437 100644 --- a/include/classes/Variable.h +++ b/include/classes/Variable.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/file_manager/Initialization.h b/include/file_manager/Initialization.h index 9678d5e1..87bb7981 100644 --- a/include/file_manager/Initialization.h +++ b/include/file_manager/Initialization.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/file_manager/InputInterpolation.h b/include/file_manager/InputInterpolation.h index 0330df32..9f1fb11d 100644 --- a/include/file_manager/InputInterpolation.h +++ b/include/file_manager/InputInterpolation.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/file_manager/InputReading.h b/include/file_manager/InputReading.h index d8d8e166..2541b665 100644 --- a/include/file_manager/InputReading.h +++ b/include/file_manager/InputReading.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/file_manager/TimeStepCalculation.h b/include/file_manager/TimeStepCalculation.h index 9dd92411..79059402 100644 --- a/include/file_manager/TimeStepCalculation.h +++ b/include/file_manager/TimeStepCalculation.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/models/GasDiffusion.h b/include/models/GasDiffusion.h index 92e7cbf4..17c96094 100644 --- a/include/models/GasDiffusion.h +++ b/include/models/GasDiffusion.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/models/StoichiometryDeviation.h b/include/models/StoichiometryDeviation.h index 6044d37e..2f10a5f2 100644 --- a/include/models/StoichiometryDeviation.h +++ b/include/models/StoichiometryDeviation.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/namespaces/Constants.h b/include/namespaces/Constants.h index 36c32cdf..132dc3e7 100644 --- a/include/namespaces/Constants.h +++ b/include/namespaces/Constants.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/namespaces/ErrorMessages.h b/include/namespaces/ErrorMessages.h index fbdd9b61..b3b4ea2e 100644 --- a/include/namespaces/ErrorMessages.h +++ b/include/namespaces/ErrorMessages.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/operations/SetGas.h b/include/operations/SetGas.h index bdb6e8ca..afd0ef35 100644 --- a/include/operations/SetGas.h +++ b/include/operations/SetGas.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/operations/SetMatrix.h b/include/operations/SetMatrix.h index 46d734ab..f41271d3 100644 --- a/include/operations/SetMatrix.h +++ b/include/operations/SetMatrix.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/operations/SetSystem.h b/include/operations/SetSystem.h index fc085aa5..68d3beac 100644 --- a/include/operations/SetSystem.h +++ b/include/operations/SetSystem.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/operations/SetVariables.h b/include/operations/SetVariables.h index 3d496ba8..7cb5f6ff 100644 --- a/include/operations/SetVariables.h +++ b/include/operations/SetVariables.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/include/operations/SetVariablesFunctions.h b/include/operations/SetVariablesFunctions.h index 08ebcc48..76a2657c 100644 --- a/include/operations/SetVariablesFunctions.h +++ b/include/operations/SetVariablesFunctions.h @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/MainSCIANTIX.C b/src/MainSCIANTIX.C index 1c852cdb..b1dc8e66 100644 --- a/src/MainSCIANTIX.C +++ b/src/MainSCIANTIX.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/MainVariables.C b/src/MainVariables.C index 068f7211..6b8eb155 100644 --- a/src/MainVariables.C +++ b/src/MainVariables.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/Sciantix.C b/src/Sciantix.C index 4c43e396..1d19ecbd 100644 --- a/src/Sciantix.C +++ b/src/Sciantix.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/classes/Matrix.C b/src/classes/Matrix.C index a9ac54c1..609fd3f2 100644 --- a/src/classes/Matrix.C +++ b/src/classes/Matrix.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/classes/SciantixVariable.C b/src/classes/SciantixVariable.C index a0cf7703..8dfabd8a 100644 --- a/src/classes/SciantixVariable.C +++ b/src/classes/SciantixVariable.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/classes/Simulation.C b/src/classes/Simulation.C index c9793586..8ba0e44b 100644 --- a/src/classes/Simulation.C +++ b/src/classes/Simulation.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/classes/Solver.C b/src/classes/Solver.C index 0d59b656..39f5915b 100644 --- a/src/classes/Solver.C +++ b/src/classes/Solver.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/classes/System.C b/src/classes/System.C index 38bba7c3..40178ebf 100644 --- a/src/classes/System.C +++ b/src/classes/System.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/file_manager/Initialization.C b/src/file_manager/Initialization.C index 11ecb7dc..089db1ea 100644 --- a/src/file_manager/Initialization.C +++ b/src/file_manager/Initialization.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/file_manager/InputInterpolation.C b/src/file_manager/InputInterpolation.C index a819e475..10effc90 100644 --- a/src/file_manager/InputInterpolation.C +++ b/src/file_manager/InputInterpolation.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/file_manager/InputReading.C b/src/file_manager/InputReading.C index b1bcd8de..207eaf0c 100644 --- a/src/file_manager/InputReading.C +++ b/src/file_manager/InputReading.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/file_manager/Output.C b/src/file_manager/Output.C index 12fb4267..f7f274eb 100644 --- a/src/file_manager/Output.C +++ b/src/file_manager/Output.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/file_manager/TimeStepCalculation.C b/src/file_manager/TimeStepCalculation.C index 48b14473..b384681d 100644 --- a/src/file_manager/TimeStepCalculation.C +++ b/src/file_manager/TimeStepCalculation.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/Burnup.C b/src/models/Burnup.C index eaf6cd1d..a10ea84c 100644 --- a/src/models/Burnup.C +++ b/src/models/Burnup.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/EffectiveBurnup.C b/src/models/EffectiveBurnup.C index 8446f80c..20684ff8 100644 --- a/src/models/EffectiveBurnup.C +++ b/src/models/EffectiveBurnup.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GapPartialPressure.C b/src/models/GapPartialPressure.C index 72ecd0f2..7f87a7e5 100644 --- a/src/models/GapPartialPressure.C +++ b/src/models/GapPartialPressure.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GasDecay.C b/src/models/GasDecay.C index 08459cd0..947343a1 100644 --- a/src/models/GasDecay.C +++ b/src/models/GasDecay.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GasDiffusion.C b/src/models/GasDiffusion.C index 57c9a049..bf132d94 100644 --- a/src/models/GasDiffusion.C +++ b/src/models/GasDiffusion.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GasProduction.C b/src/models/GasProduction.C index aa3cbf1d..76ab8b1c 100644 --- a/src/models/GasProduction.C +++ b/src/models/GasProduction.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GrainBoundaryMicroCracking.C b/src/models/GrainBoundaryMicroCracking.C index 1999ad98..b70c2548 100644 --- a/src/models/GrainBoundaryMicroCracking.C +++ b/src/models/GrainBoundaryMicroCracking.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GrainBoundarySweeping.C b/src/models/GrainBoundarySweeping.C index 7ded7e49..cb06e9f2 100644 --- a/src/models/GrainBoundarySweeping.C +++ b/src/models/GrainBoundarySweeping.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GrainBoundaryVenting.C b/src/models/GrainBoundaryVenting.C index 425ec633..21654f2e 100644 --- a/src/models/GrainBoundaryVenting.C +++ b/src/models/GrainBoundaryVenting.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/GrainGrowth.C b/src/models/GrainGrowth.C index 415aac62..c3b520d9 100644 --- a/src/models/GrainGrowth.C +++ b/src/models/GrainGrowth.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/HighBurnupStructureFormation.C b/src/models/HighBurnupStructureFormation.C index c52b1d44..c4b9035f 100644 --- a/src/models/HighBurnupStructureFormation.C +++ b/src/models/HighBurnupStructureFormation.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/HighBurnupStructurePorosity.C b/src/models/HighBurnupStructurePorosity.C index 21f37917..d39d551e 100644 --- a/src/models/HighBurnupStructurePorosity.C +++ b/src/models/HighBurnupStructurePorosity.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/InterGranularBubbleBehavior.C b/src/models/InterGranularBubbleBehavior.C index a5e6d433..203aef4a 100644 --- a/src/models/InterGranularBubbleBehavior.C +++ b/src/models/InterGranularBubbleBehavior.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/IntraGranularBubbleBehaviour.C b/src/models/IntraGranularBubbleBehaviour.C index 590a115b..32ecc0fd 100644 --- a/src/models/IntraGranularBubbleBehaviour.C +++ b/src/models/IntraGranularBubbleBehaviour.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/StoichiometryDeviation.C b/src/models/StoichiometryDeviation.C index f430d804..78e5da94 100644 --- a/src/models/StoichiometryDeviation.C +++ b/src/models/StoichiometryDeviation.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/models/UO2Thermochemistry.C b/src/models/UO2Thermochemistry.C index 44aa7e63..67320e78 100644 --- a/src/models/UO2Thermochemistry.C +++ b/src/models/UO2Thermochemistry.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/namespaces/ErrorMessages.C b/src/namespaces/ErrorMessages.C index 691b1ce7..85929544 100644 --- a/src/namespaces/ErrorMessages.C +++ b/src/namespaces/ErrorMessages.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/operations/SetGas.C b/src/operations/SetGas.C index e5a5e3a4..d6c01aea 100644 --- a/src/operations/SetGas.C +++ b/src/operations/SetGas.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/operations/SetMatrix.C b/src/operations/SetMatrix.C index d811f1ec..acde0a84 100644 --- a/src/operations/SetMatrix.C +++ b/src/operations/SetMatrix.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/operations/SetSystem.C b/src/operations/SetSystem.C index 4555f6cd..7b6d76c5 100644 --- a/src/operations/SetSystem.C +++ b/src/operations/SetSystem.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/operations/SetVariables.C b/src/operations/SetVariables.C index 41216b97..3d25b850 100644 --- a/src/operations/SetVariables.C +++ b/src/operations/SetVariables.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// diff --git a/src/operations/UpdateVariables.C b/src/operations/UpdateVariables.C index 75c3d732..c6060c43 100644 --- a/src/operations/UpdateVariables.C +++ b/src/operations/UpdateVariables.C @@ -9,7 +9,7 @@ // Originally developed by D. Pizzocri & T. Barani // // // // Version: 2.1 // -// Year: 2023 // +// Year: 2024 // // Authors: D. Pizzocri, G. Zullo. // // // ////////////////////////////////////////////////////////////////////////////////////// From 106ae2ce45eece74876fa3fa290a71201db1c108 Mon Sep 17 00:00:00 2001 From: giozu Date: Mon, 26 Aug 2024 18:49:30 +0200 Subject: [PATCH 02/15] docs update --- docs/_constants_8h_source.html | 2 +- docs/_error_messages_8h_source.html | 2 +- docs/_gas_8h_source.html | 2 +- docs/_gas_diffusion_8h_source.html | 2 +- docs/_initialization_8h_source.html | 2 +- docs/_input_interpolation_8h_source.html | 2 +- docs/_input_reading_8h_source.html | 2 +- docs/_input_variable_8h_source.html | 2 +- docs/_main_variables_8h_source.html | 2 +- docs/_material_8h_source.html | 2 +- docs/_matrix_8h_source.html | 2 +- docs/_model_8h_source.html | 2 +- docs/_sciantix_8h_source.html | 2 +- docs/_sciantix_array_8h_source.html | 2 +- docs/_sciantix_variable_8h_source.html | 2 +- docs/_set_gas_8h_source.html | 2 +- docs/_set_matrix_8h_source.html | 2 +- docs/_set_system_8h_source.html | 2 +- docs/_set_variables_8h_source.html | 2 +- docs/_set_variables_functions_8h_source.html | 2 +- docs/_simulation_8h_source.html | 2 +- docs/_solver_8h_source.html | 2 +- docs/_stoichiometry_deviation_8h_source.html | 2 +- docs/_system_8h_source.html | 2 +- docs/_time_step_calculation_8h_source.html | 2 +- docs/_variable_8h_source.html | 2 +- 26 files changed, 26 insertions(+), 26 deletions(-) diff --git a/docs/_constants_8h_source.html b/docs/_constants_8h_source.html index c8061adf..eb509e90 100644 --- a/docs/_constants_8h_source.html +++ b/docs/_constants_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_error_messages_8h_source.html b/docs/_error_messages_8h_source.html index a42b7b32..2c7a5a49 100644 --- a/docs/_error_messages_8h_source.html +++ b/docs/_error_messages_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_gas_8h_source.html b/docs/_gas_8h_source.html index d300cf20..eae23077 100644 --- a/docs/_gas_8h_source.html +++ b/docs/_gas_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
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16 
diff --git a/docs/_gas_diffusion_8h_source.html b/docs/_gas_diffusion_8h_source.html index 1b9f4e9e..db33880b 100644 --- a/docs/_gas_diffusion_8h_source.html +++ b/docs/_gas_diffusion_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
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12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_initialization_8h_source.html b/docs/_initialization_8h_source.html index cdf2d140..794c39dc 100644 --- a/docs/_initialization_8h_source.html +++ b/docs/_initialization_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
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13 // Authors: D. Pizzocri, G. Zullo. //
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diff --git a/docs/_input_interpolation_8h_source.html b/docs/_input_interpolation_8h_source.html index d3936a08..6c108d24 100644 --- a/docs/_input_interpolation_8h_source.html +++ b/docs/_input_interpolation_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_input_reading_8h_source.html b/docs/_input_reading_8h_source.html index ea6bb8ee..eb2c4a33 100644 --- a/docs/_input_reading_8h_source.html +++ b/docs/_input_reading_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_input_variable_8h_source.html b/docs/_input_variable_8h_source.html index 7aca478b..f9d241c1 100644 --- a/docs/_input_variable_8h_source.html +++ b/docs/_input_variable_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_main_variables_8h_source.html b/docs/_main_variables_8h_source.html index 90823f11..276938f5 100644 --- a/docs/_main_variables_8h_source.html +++ b/docs/_main_variables_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_material_8h_source.html b/docs/_material_8h_source.html index d2bbc429..7ff8b71e 100644 --- a/docs/_material_8h_source.html +++ b/docs/_material_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_matrix_8h_source.html b/docs/_matrix_8h_source.html index a84b3052..fe32a987 100644 --- a/docs/_matrix_8h_source.html +++ b/docs/_matrix_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_model_8h_source.html b/docs/_model_8h_source.html index bb5decf8..aa21efd1 100644 --- a/docs/_model_8h_source.html +++ b/docs/_model_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
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12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
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16 
diff --git a/docs/_sciantix_8h_source.html b/docs/_sciantix_8h_source.html index 75e6574d..f5eb6ce3 100644 --- a/docs/_sciantix_8h_source.html +++ b/docs/_sciantix_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
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12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_sciantix_array_8h_source.html b/docs/_sciantix_array_8h_source.html index 39c64fa3..70c1dc73 100644 --- a/docs/_sciantix_array_8h_source.html +++ b/docs/_sciantix_array_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
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12 // Year: 2023 //
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13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
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diff --git a/docs/_sciantix_variable_8h_source.html b/docs/_sciantix_variable_8h_source.html index 21b06f99..94500200 100644 --- a/docs/_sciantix_variable_8h_source.html +++ b/docs/_sciantix_variable_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_set_gas_8h_source.html b/docs/_set_gas_8h_source.html index bd8c5533..b35b1578 100644 --- a/docs/_set_gas_8h_source.html +++ b/docs/_set_gas_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_set_matrix_8h_source.html b/docs/_set_matrix_8h_source.html index 14b02421..0e20e58b 100644 --- a/docs/_set_matrix_8h_source.html +++ b/docs/_set_matrix_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
-
12 // Year: 2023 //
+
12 // Year: 2024 //
13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_set_system_8h_source.html b/docs/_set_system_8h_source.html index 72e0e65b..321c5833 100644 --- a/docs/_set_system_8h_source.html +++ b/docs/_set_system_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
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13 // Authors: D. Pizzocri, G. Zullo. //
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diff --git a/docs/_set_variables_8h_source.html b/docs/_set_variables_8h_source.html index 2f19d12f..6282b812 100644 --- a/docs/_set_variables_8h_source.html +++ b/docs/_set_variables_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
11 // Version: 2.1 //
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12 // Year: 2023 //
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13 // Authors: D. Pizzocri, G. Zullo. //
14 // //
16 
diff --git a/docs/_set_variables_functions_8h_source.html b/docs/_set_variables_functions_8h_source.html index c932d5aa..4e44a4e3 100644 --- a/docs/_set_variables_functions_8h_source.html +++ b/docs/_set_variables_functions_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
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13 // Authors: D. Pizzocri, G. Zullo. //
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diff --git a/docs/_simulation_8h_source.html b/docs/_simulation_8h_source.html index 121c4300..fab8788b 100644 --- a/docs/_simulation_8h_source.html +++ b/docs/_simulation_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
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13 // Authors: D. Pizzocri, G. Zullo. //
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diff --git a/docs/_solver_8h_source.html b/docs/_solver_8h_source.html index 629c9524..783a5aa3 100644 --- a/docs/_solver_8h_source.html +++ b/docs/_solver_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
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13 // Authors: D. Pizzocri, G. Zullo. //
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diff --git a/docs/_stoichiometry_deviation_8h_source.html b/docs/_stoichiometry_deviation_8h_source.html index bd2e5327..8f46efad 100644 --- a/docs/_stoichiometry_deviation_8h_source.html +++ b/docs/_stoichiometry_deviation_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
10 // //
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13 // Authors: D. Pizzocri, G. Zullo. //
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diff --git a/docs/_system_8h_source.html b/docs/_system_8h_source.html index b2a824f0..a2918bcb 100644 --- a/docs/_system_8h_source.html +++ b/docs/_system_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
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diff --git a/docs/_time_step_calculation_8h_source.html b/docs/_time_step_calculation_8h_source.html index a58b6f9b..2cb9299f 100644 --- a/docs/_time_step_calculation_8h_source.html +++ b/docs/_time_step_calculation_8h_source.html @@ -80,7 +80,7 @@
9 // Originally developed by D. Pizzocri & T. Barani //
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13 // Authors: D. Pizzocri, G. Zullo. //
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9 // Originally developed by D. Pizzocri & T. Barani //
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From 979fdac9c9be3ea56f2a1901638a1fafea6bca53 Mon Sep 17 00:00:00 2001 From: giozu Date: Tue, 27 Aug 2024 15:15:54 +0200 Subject: [PATCH 03/15] file formatting --- Doxyfile | 2 +- docs/_simulation_8h_source.html | 2 +- docs/_system_8h_source.html | 2 +- docs/class_simulation.html | 67 +--- include/models/GasDiffusion.h | 2 +- regression/regression_baker.py | 76 ++--- regression/test_Baker1977__1273K/overview.txt | 4 - regression/test_Baker1977__1373K/overview.txt | 4 - regression/test_Baker1977__1473K/overview.txt | 4 - regression/test_Baker1977__1573K/overview.txt | 4 - regression/test_Baker1977__1673K/overview.txt | 4 - regression/test_Baker1977__1773K/overview.txt | 4 - regression/test_Baker1977__1873K/overview.txt | 4 - regression/test_Baker1977__1973K/overview.txt | 4 - regression/test_Baker1977__2073K/overview.txt | 4 - regression/test_CONTACT1/overview.txt | 4 - regression/test_Kashibe1993_23/overview.txt | 4 - regression/test_Kashibe1993_44/overview.txt | 4 - regression/test_Talip2014_1320K/overview.txt | 3 - .../test_Talip2014_1400K_b/overview.txt | 3 - .../test_Talip2014_1400K_c/overview.txt | 3 - regression/test_Talip2014_1600K/overview.txt | 3 - regression/test_Talip2014_1800K/overview.txt | 3 - regression/test_UO2HBS/overview.txt | 2 - .../overview.txt | 4 - .../overview.txt | 4 - .../overview.txt | 4 - .../test_UO2_oxidation_PS-623C/overview.txt | 4 - regression/test_White2004_4000-1/overview.txt | 4 - regression/test_White2004_4000-2/overview.txt | 4 - regression/test_White2004_4000-3/overview.txt | 4 - regression/test_White2004_4000-4/overview.txt | 4 - regression/test_White2004_4000-5/overview.txt | 4 - regression/test_White2004_4004-1/overview.txt | 4 - regression/test_White2004_4004-2/overview.txt | 4 - regression/test_White2004_4004-3/overview.txt | 4 - regression/test_White2004_4004-4/overview.txt | 4 - regression/test_White2004_4004-5/overview.txt | 4 - regression/test_White2004_4004-6/overview.txt | 4 - regression/test_White2004_4005-1/overview.txt | 4 - regression/test_White2004_4005-2/overview.txt | 4 - regression/test_White2004_4005-3/overview.txt | 4 - regression/test_White2004_4005-4/overview.txt | 4 - regression/test_White2004_4005-5/overview.txt | 4 - regression/test_White2004_4064-1/overview.txt | 4 - regression/test_White2004_4064-2/overview.txt | 4 - regression/test_White2004_4064-3/overview.txt | 4 - regression/test_White2004_4064-4/overview.txt | 4 - regression/test_White2004_4064-5/overview.txt | 4 - regression/test_White2004_4065-1/overview.txt | 4 - regression/test_White2004_4065-2/overview.txt | 4 - regression/test_White2004_4065-3/overview.txt | 4 - regression/test_White2004_4065-4/overview.txt | 4 - regression/test_White2004_4065-5/overview.txt | 4 - regression/test_White2004_4135-1/overview.txt | 4 - regression/test_White2004_4135-2/overview.txt | 4 - regression/test_White2004_4135-3/overview.txt | 4 - regression/test_White2004_4136-1/overview.txt | 4 - regression/test_White2004_4136-2/overview.txt | 4 - regression/test_White2004_4136-3/overview.txt | 4 - regression/test_White2004_4136-4/overview.txt | 4 - regression/test_White2004_4140-1/overview.txt | 4 - regression/test_White2004_4140-2/overview.txt | 4 - regression/test_White2004_4162-1/overview.txt | 4 - regression/test_White2004_4162-2/overview.txt | 4 - regression/test_White2004_4162-3/overview.txt | 4 - regression/test_White2004_4162-4/overview.txt | 4 - regression/test_White2004_4163-1/overview.txt | 4 - regression/test_White2004_4163-2/overview.txt | 4 - regression/test_White2004_4163-3/overview.txt | 4 - regression/test_White2004_4163-4/overview.txt | 4 - src/classes/System.C | 4 +- src/models/Burnup.C | 2 +- src/models/EffectiveBurnup.C | 18 +- src/models/GapPartialPressure.C | 1 + src/models/GasDecay.C | 1 + src/models/GasDiffusion.C | 237 +++++++------- src/models/GasProduction.C | 31 +- src/models/GrainBoundaryMicroCracking.C | 79 ++--- src/models/GrainBoundarySweeping.C | 150 +++++---- src/models/GrainBoundaryVenting.C | 87 ++--- src/models/GrainGrowth.C | 149 ++++----- src/models/HighBurnupStructureFormation.C | 100 +++--- src/models/HighBurnupStructurePorosity.C | 175 +++++------ src/models/InterGranularBubbleBehavior.C | 297 +++++++++--------- src/models/IntraGranularBubbleBehavior.C | 153 +++++++++ src/models/IntraGranularBubbleBehaviour.C | 187 ----------- src/models/StoichiometryDeviation.C | 4 +- 88 files changed, 859 insertions(+), 1220 deletions(-) create mode 100644 src/models/IntraGranularBubbleBehavior.C delete mode 100644 src/models/IntraGranularBubbleBehaviour.C diff --git a/Doxyfile b/Doxyfile index e47bbdf3..fa066e1e 100644 --- a/Doxyfile +++ b/Doxyfile @@ -1,6 +1,6 @@ # Doxyfile for SCIANTIX repository # -# Author: G. Zullo (feel free to write to: giovanni.zullo@polimi.it) +# Author: G. Zullo (giovanni.zullo@polimi.it) # Date: May 2022 # # Instructions: diff --git a/docs/_simulation_8h_source.html b/docs/_simulation_8h_source.html index fab8788b..efbc4f96 100644 --- a/docs/_simulation_8h_source.html +++ b/docs/_simulation_8h_source.html @@ -268,7 +268,7 @@
Simulation
Derived class that orchestrates the overall simulation process combining various models and solvers.
Definition: Simulation.h:41
Simulation::GasProduction
void GasProduction()
GasProduction computes the gas produced from the production rate.
Definition: GasProduction.C:19
Simulation::GrainBoundaryMicroCracking
void GrainBoundaryMicroCracking()
GrainBoundaryMicroCracking is method of simulation which executes the SCIANTIX simulation for the gra...
Definition: GrainBoundaryMicroCracking.C:19
-
Simulation::IntraGranularBubbleBehavior
void IntraGranularBubbleBehavior()
Evolution models for intra-granular bubbles in fuel grains based on the value of iIntraGranularBubble...
Definition: IntraGranularBubbleBehaviour.C:19
+
Simulation::IntraGranularBubbleBehavior
void IntraGranularBubbleBehavior()
Evolution models for intra-granular bubbles in fuel grains based on the value of iIntraGranularBubble...
Definition: IntraGranularBubbleBehavior.C:19
Simulation::EffectiveBurnup
void EffectiveBurnup()
EffectiveBurnup () calculates the local effective burnup of the fuel.
Definition: EffectiveBurnup.C:19
Simulation::InterGranularBubbleBehavior
void InterGranularBubbleBehavior()
The model considers one-off nucleation, growth of lenticular bubbles by vacancy absorption and coales...
Definition: InterGranularBubbleBehavior.C:19
Simulation::Burnup
void Burnup()
Burnup() calculates the local burnup from fission rate and fuel density.
Definition: Burnup.C:19
diff --git a/docs/_system_8h_source.html b/docs/_system_8h_source.html index a2918bcb..3f9cd487 100644 --- a/docs/_system_8h_source.html +++ b/docs/_system_8h_source.html @@ -209,7 +209,7 @@
System::~System
~System()
Destructor for the System class.
Definition: System.h:260
System::setVolumeInLattice
void setVolumeInLattice(double v)
Sets the volume occupied by the gas in the matrix.
Definition: System.C:93
System::getFissionGasDiffusivity
double getFissionGasDiffusivity()
Retrieves the diffusivity of fission gases within the matrix.
Definition: System.C:405
-
System::getProductionRate
double getProductionRate()
Member function to get the production rate of the sciantix_system.
Definition: System.C:788
+
System::getProductionRate
double getProductionRate()
Member function to get the production rate of the sciantix_system.
Definition: System.C:790
System::getHenryConstant
double getHenryConstant()
Retrieves the Henry's constant value.
Definition: System.C:417
System::getRadiusInLattice
double getRadiusInLattice()
Gets the radius of the fission gas atom in the matrix lattice.
Definition: System.C:47
System::getYield
double getYield()
Gets the cumulative yield of the fission gas.
Definition: System.C:35
diff --git a/docs/class_simulation.html b/docs/class_simulation.html index 22f09951..588b01fc 100644 --- a/docs/class_simulation.html +++ b/docs/class_simulation.html @@ -294,7 +294,7 @@

Parameters
@@ -509,21 +509,6 @@

-iHighBurnupStructureFormation == 0

-

No HBS forming in the UO2 fuel matrix.

-

-iHighBurnupStructureFormation == 1

-

This case calculates the fraction of HBS-restructured volume of the UO2 fuel matrix based on the KJMA approach.

See also
Barani et al. Journal of Nuclear Materials 539 (2020) 152296.
-
Parameters
-
[out]grain_sweeped_volume
- - - - -
[out]avrami_constant
[out]transformation_rate
[out]resolution_layer_thickness
[out]resolution_critical_distance
-
- @@ -548,8 +533,6 @@

-iIntraGranularBubbleBehavior == 1

-

The evolution of small intra-granular bubbles in fuel grains is controlled by bubble nucleation, gas atom trapping, and irradiation-induced gas atom re-solution back in the lattice.

See also
Description of the model in Pizzocri et al., JNM, 502 (2018) 323-330.
-
Parameters
- - - - - -
[out]intragranular_bubble_concentration
[out]intragranular_bubble_radius
[in]resolution_rate
[in]nucleation_rate
-
-
-

-iIntraGranularBubbleBehavior == 2

-

The evolution of intragranular bubbles is modelled by means of temperature-driven correlations.

See also
Description of the model in White, Tucker, Journal of Nuclear Materials, 118 (1983), 1-38.
-
Parameters
- - -
[in]local_fuel_temperature
-
-
-

iIntraGranularBubbleBehavior == 3

-

The evolution of intragranular bubble concentration, radius and atoms per bubble is described through the similarity ratio, based on the evolution of intragranular concentration of gas in bubbles.

-

iIntraGranularBubbleBehavior == 99 No intragranular bubbles.

-

To be used with iTrappingRate = 99, iResolutionRate = 99, iNucleationRate = 99.

-
Parameters
- - - -
[out]intragranular_bubble_radius
[out]intragranular_bubble_concentration
-
-
@@ -678,7 +629,7 @@

+

iStoichiometryDeviation = 1

Range of utilization:

  • Pure steam
    • @@ -686,7 +637,7 @@

The model for fuel oxidation and stoichimetry deviation evolution is described with a semi-empirical model. Carter and Lay, J. Nucl. Mater., 36:77–86, 1970. The oxidation rate follows: dx/dt = alpha*(S/V)*[x_eq - x]*(Ph2o^0.5)

alpha is the surface exchange coefficient for unirradiated UO2 oxidation obtained by experimments. It is expressed as alpha = A exp(−Q/T). S/V = 3/a (1/m), surface-to-volume ratio of the fuel sample x_eq : equilbrium stoichiometry deviation (evaluated by UO2Thermochemistry model)

-

+

iStoichiometryDeviation = 2

Range of utilization:

  • Pure steam
    • @@ -694,7 +645,7 @@

The model for fuel oxidation and stoichimetry deviation evolution is described with a semi-empirical model. Carter and Lay, J. Nucl. Mater., 36:77–86, 1970. The oxidation rate follows: dx/dt = alpha*(S/V)*[x_eq - x]*(Ph2o^0.5)

alpha is the surface exchange coefficient for unirradiated UO2 oxidation obtained by experimments. It is expressed as alpha = A exp(−Q/T). S/V = 3/a (1/m), surface-to-volume ratio of the fuel sample x_eq : equilbrium stoichiometry deviation (evaluated by UO2Thermochemistry model)

-

+

iStoichiometryDeviation = 3

Range of utilization:

  • Pure steam
    • @@ -703,21 +654,21 @@

The model for fuel oxidation and stoichimetry deviation evolution is described with a semi-empirical model. Carter and Lay, J. Nucl. Mater., 36:77–86, 1970. The oxidation rate follows: dx/dt = alpha*(S/V)*[x_eq - x]*(Ph2o^0.5)

alpha is the surface exchange coefficient for unirradiated UO2 oxidation obtained by experiments. It is expressed as alpha = A exp(−Q/T). S/V = 3/a (1/m), surface-to-volume ratio of the fuel sample x_eq : equilbrium stoichiometry deviation (evaluated by UO2Thermochemistry model)

-

+

iStoichiometryDeviation = 4

Range of utilization:

  • Pure steam
  • Temperature range: 1073-1473 Imamura and. Une, JNM, 247:131–137, 1997.

The model for fuel oxidation and stoichimetry deviation evolution is described with a mechanistic Langmuir-based approach Massih, A. R. "UO2 fuel oxidation and fission gas release." Swedish Radiation Safety Authority report, Report 2018 (2018): 25. The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x))

-

+

iStoichiometryDeviation = 5

Range of utilization:

  • Pure steam
  • Temperature range: 1073-1673 K

The model for fuel oxidation and stoichimetry deviation evolution is described with a mechanistic Langmuir-based approach Massih, A. R. "UO2 fuel oxidation and fission gas release." Swedish Radiation Safety Authority report, Report 2018 (2018): 25. The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x))

-

+

iStoichiometryDeviation = 5

Range of utilization:

-

The model for fuel oxidation and stoichimetry deviation evolution is described with a mechanistic Langmuir-based approach Massih, A. R. "UO2 fuel oxidation and fission gas release." Swedish Radiation Safety Authority report, Report 2018 (2018): 25. The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x))

+

The model for fuel oxidation and stoichimetry deviation evolution is described with a mechanistic Langmuir-based approach Massih A.R. (2018). UO2 Fuel Oxidation and Fission Gas Release, Swedish Radiation Safety Authority (SSM). The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x))

iStoichiometryDeviation = 5

Range of utilization:

  • Pure steam
  • Temperature range: 1073-1673 K
-

The model for fuel oxidation and stoichimetry deviation evolution is described with a mechanistic Langmuir-based approach Massih, A. R. "UO2 fuel oxidation and fission gas release." Swedish Radiation Safety Authority report, Report 2018 (2018): 25. The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x))

+

The model for fuel oxidation and stoichimetry deviation evolution is described with a mechanistic Langmuir-based approach Massih A.R. (2018). UO2 Fuel Oxidation and Fission Gas Release, Swedish Radiation Safety Authority (SSM). The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x))

-iStoichiometryDeviation = 5

+iStoichiometryDeviation = 6

Range of utilization:

  • Pure steam
  • Temperature range: 1073-1673 K
    • diff --git a/regression/test_Baker1977__1273K/overview.txt b/regression/test_Baker1977__1273K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1273K/overview.txt +++ b/regression/test_Baker1977__1273K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__1373K/overview.txt b/regression/test_Baker1977__1373K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1373K/overview.txt +++ b/regression/test_Baker1977__1373K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__1473K/overview.txt b/regression/test_Baker1977__1473K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1473K/overview.txt +++ b/regression/test_Baker1977__1473K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__1573K/overview.txt b/regression/test_Baker1977__1573K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1573K/overview.txt +++ b/regression/test_Baker1977__1573K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__1673K/overview.txt b/regression/test_Baker1977__1673K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1673K/overview.txt +++ b/regression/test_Baker1977__1673K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__1773K/overview.txt b/regression/test_Baker1977__1773K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1773K/overview.txt +++ b/regression/test_Baker1977__1773K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__1873K/overview.txt b/regression/test_Baker1977__1873K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1873K/overview.txt +++ b/regression/test_Baker1977__1873K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__1973K/overview.txt b/regression/test_Baker1977__1973K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__1973K/overview.txt +++ b/regression/test_Baker1977__1973K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Baker1977__2073K/overview.txt b/regression/test_Baker1977__2073K/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Baker1977__2073K/overview.txt +++ b/regression/test_Baker1977__2073K/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_CONTACT1/overview.txt b/regression/test_CONTACT1/overview.txt index 328e1d58..96766305 100644 --- a/regression/test_CONTACT1/overview.txt +++ b/regression/test_CONTACT1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from White, JNM, 325 (2004), 61-77. diff --git a/regression/test_Kashibe1993_23/overview.txt b/regression/test_Kashibe1993_23/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Kashibe1993_23/overview.txt +++ b/regression/test_Kashibe1993_23/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Kashibe1993_44/overview.txt b/regression/test_Kashibe1993_44/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_Kashibe1993_44/overview.txt +++ b/regression/test_Kashibe1993_44/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Talip2014_1320K/overview.txt b/regression/test_Talip2014_1320K/overview.txt index abeaebf4..186e2731 100644 --- a/regression/test_Talip2014_1320K/overview.txt +++ b/regression/test_Talip2014_1320K/overview.txt @@ -16,7 +16,7 @@ Model Gas diffusion - Kr85m in UO2 Model Intergranular bubble behavior : No model for grain-boundary bubble evolution. Matrix UO2 - : Van Uffelen et al. JNM, 434 (2013) 287-29. + Van Uffelen et al. JNM, 434 (2013) 287-29. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Talip2014_1400K_b/overview.txt b/regression/test_Talip2014_1400K_b/overview.txt index abeaebf4..186e2731 100644 --- a/regression/test_Talip2014_1400K_b/overview.txt +++ b/regression/test_Talip2014_1400K_b/overview.txt @@ -16,7 +16,7 @@ Model Gas diffusion - Kr85m in UO2 Model Intergranular bubble behavior : No model for grain-boundary bubble evolution. Matrix UO2 - : Van Uffelen et al. JNM, 434 (2013) 287-29. + Van Uffelen et al. JNM, 434 (2013) 287-29. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Talip2014_1400K_c/overview.txt b/regression/test_Talip2014_1400K_c/overview.txt index abeaebf4..186e2731 100644 --- a/regression/test_Talip2014_1400K_c/overview.txt +++ b/regression/test_Talip2014_1400K_c/overview.txt @@ -16,7 +16,7 @@ Model Gas diffusion - Kr85m in UO2 Model Intergranular bubble behavior : No model for grain-boundary bubble evolution. Matrix UO2 - : Van Uffelen et al. JNM, 434 (2013) 287-29. + Van Uffelen et al. JNM, 434 (2013) 287-29. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Talip2014_1600K/overview.txt b/regression/test_Talip2014_1600K/overview.txt index abeaebf4..186e2731 100644 --- a/regression/test_Talip2014_1600K/overview.txt +++ b/regression/test_Talip2014_1600K/overview.txt @@ -16,7 +16,7 @@ Model Gas diffusion - Kr85m in UO2 Model Intergranular bubble behavior : No model for grain-boundary bubble evolution. Matrix UO2 - : Van Uffelen et al. JNM, 434 (2013) 287-29. + Van Uffelen et al. JNM, 434 (2013) 287-29. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_Talip2014_1800K/overview.txt b/regression/test_Talip2014_1800K/overview.txt index abeaebf4..186e2731 100644 --- a/regression/test_Talip2014_1800K/overview.txt +++ b/regression/test_Talip2014_1800K/overview.txt @@ -16,7 +16,7 @@ Model Gas diffusion - Kr85m in UO2 Model Intergranular bubble behavior : No model for grain-boundary bubble evolution. Matrix UO2 - : Van Uffelen et al. JNM, 434 (2013) 287-29. + Van Uffelen et al. JNM, 434 (2013) 287-29. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_UO2HBS/overview.txt b/regression/test_UO2HBS/overview.txt index c9e1abd5..83b611bc 100644 --- a/regression/test_UO2HBS/overview.txt +++ b/regression/test_UO2HBS/overview.txt @@ -2,20 +2,20 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. Model High-burnup structure formation : Barani et al. Journal of Nuclear Materials 539 (2020) 152296 Model High-burnup structure porosity : Based on Spino et al. 2006 data -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Xe in UO2HBS Model Intragranular bubble behavior : Pizzocri et al., JNM, 502 (2018) 323-330. Model Gas diffusion - Xe in UO2 with HBS -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. Matrix UO2HBS - : Null grain-boundary mobility. + Null grain-boundary mobility. iGrainBoundaryVacancyDiffusivity: HBS case, from Barani et al., JNM 563 (2022) 153627. diff --git a/regression/test_UO2_oxidation_Cox_et_al_data_1273K/overview.txt b/regression/test_UO2_oxidation_Cox_et_al_data_1273K/overview.txt index 49569b6a..0ee88226 100644 --- a/regression/test_UO2_oxidation_Cox_et_al_data_1273K/overview.txt +++ b/regression/test_UO2_oxidation_Cox_et_al_data_1273K/overview.txt @@ -1,8 +1,8 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model UO2 thermochemistry Blackburn (1973) J. Nucl. Mater., 46, 244-252. -Model Stoichiometry deviation -Model Grain growth constant grain radius. +Model UO2 thermochemistry : Blackburn (1973) J. Nucl. Mater., 46, 244-252. +Model Stoichiometry deviation : Massih, A. R. UO2 fuel oxidation and fission gas release. Swedish Radiation Safety Authority report, Report 2018 (2018): 25 +Model Grain growth : constant grain radius. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -14,11 +14,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Null grain-boundary mobility. + Null grain-boundary mobility. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_UO2_oxidation_Cox_et_al_data_1473K/overview.txt b/regression/test_UO2_oxidation_Cox_et_al_data_1473K/overview.txt index 49569b6a..0ee88226 100644 --- a/regression/test_UO2_oxidation_Cox_et_al_data_1473K/overview.txt +++ b/regression/test_UO2_oxidation_Cox_et_al_data_1473K/overview.txt @@ -1,8 +1,8 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model UO2 thermochemistry Blackburn (1973) J. Nucl. Mater., 46, 244-252. -Model Stoichiometry deviation -Model Grain growth constant grain radius. +Model UO2 thermochemistry : Blackburn (1973) J. Nucl. Mater., 46, 244-252. +Model Stoichiometry deviation : Massih, A. R. UO2 fuel oxidation and fission gas release. Swedish Radiation Safety Authority report, Report 2018 (2018): 25 +Model Grain growth : constant grain radius. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -14,11 +14,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Null grain-boundary mobility. + Null grain-boundary mobility. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_UO2_oxidation_Imamura_and_Une_data/overview.txt b/regression/test_UO2_oxidation_Imamura_and_Une_data/overview.txt index f0ba3753..faf911a8 100644 --- a/regression/test_UO2_oxidation_Imamura_and_Une_data/overview.txt +++ b/regression/test_UO2_oxidation_Imamura_and_Une_data/overview.txt @@ -1,8 +1,8 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model UO2 thermochemistry Blackburn (1973) J. Nucl. Mater., 46, 244-252. -Model Stoichiometry deviation Carter and Lay, J. Nucl. Mater., 36:77-86, 1970. Imamura and. Une, JNM, 247:131-137, 1997. -Model Grain growth constant grain radius. +Model UO2 thermochemistry : Blackburn (1973) J. Nucl. Mater., 46, 244-252. +Model Stoichiometry deviation : Carter and Lay, J. Nucl. Mater., 36:77-86, 1970. Imamura and. Une, JNM, 247:131-137, 1997. +Model Grain growth : constant grain radius. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -14,11 +14,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Null grain-boundary mobility. + Null grain-boundary mobility. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_UO2_oxidation_PS-623C/overview.txt b/regression/test_UO2_oxidation_PS-623C/overview.txt index eababe5d..6f8a2bb4 100644 --- a/regression/test_UO2_oxidation_PS-623C/overview.txt +++ b/regression/test_UO2_oxidation_PS-623C/overview.txt @@ -1,8 +1,8 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model UO2 thermochemistry Blackburn (1973) J. Nucl. Mater., 46, 244-252. -Model Stoichiometry deviation Carter and Lay, J. Nucl. Mater., 36:77-86, 1970. Abrefah, JNM., 208:98-110, 1994. -Model Grain growth constant grain radius. +Model UO2 thermochemistry : Blackburn (1973) J. Nucl. Mater., 46, 244-252. +Model Stoichiometry deviation : Carter and Lay, J. Nucl. Mater., 36:77-86, 1970. Abrefah, JNM., 208:98-110, 1994. +Model Grain growth : constant grain radius. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -14,11 +14,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Null grain-boundary mobility. + Null grain-boundary mobility. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4000-1/overview.txt b/regression/test_White2004_4000-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4000-1/overview.txt +++ b/regression/test_White2004_4000-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4000-2/overview.txt b/regression/test_White2004_4000-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4000-2/overview.txt +++ b/regression/test_White2004_4000-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4000-3/overview.txt b/regression/test_White2004_4000-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4000-3/overview.txt +++ b/regression/test_White2004_4000-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4000-4/overview.txt b/regression/test_White2004_4000-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4000-4/overview.txt +++ b/regression/test_White2004_4000-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4000-5/overview.txt b/regression/test_White2004_4000-5/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4000-5/overview.txt +++ b/regression/test_White2004_4000-5/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4004-1/overview.txt b/regression/test_White2004_4004-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4004-1/overview.txt +++ b/regression/test_White2004_4004-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4004-2/overview.txt b/regression/test_White2004_4004-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4004-2/overview.txt +++ b/regression/test_White2004_4004-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4004-3/overview.txt b/regression/test_White2004_4004-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4004-3/overview.txt +++ b/regression/test_White2004_4004-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4004-4/overview.txt b/regression/test_White2004_4004-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4004-4/overview.txt +++ b/regression/test_White2004_4004-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4004-5/overview.txt b/regression/test_White2004_4004-5/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4004-5/overview.txt +++ b/regression/test_White2004_4004-5/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4004-6/overview.txt b/regression/test_White2004_4004-6/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4004-6/overview.txt +++ b/regression/test_White2004_4004-6/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4005-1/overview.txt b/regression/test_White2004_4005-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4005-1/overview.txt +++ b/regression/test_White2004_4005-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4005-2/overview.txt b/regression/test_White2004_4005-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4005-2/overview.txt +++ b/regression/test_White2004_4005-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4005-3/overview.txt b/regression/test_White2004_4005-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4005-3/overview.txt +++ b/regression/test_White2004_4005-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4005-4/overview.txt b/regression/test_White2004_4005-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4005-4/overview.txt +++ b/regression/test_White2004_4005-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4005-5/overview.txt b/regression/test_White2004_4005-5/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4005-5/overview.txt +++ b/regression/test_White2004_4005-5/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4064-1/overview.txt b/regression/test_White2004_4064-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4064-1/overview.txt +++ b/regression/test_White2004_4064-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4064-2/overview.txt b/regression/test_White2004_4064-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4064-2/overview.txt +++ b/regression/test_White2004_4064-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4064-3/overview.txt b/regression/test_White2004_4064-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4064-3/overview.txt +++ b/regression/test_White2004_4064-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4064-4/overview.txt b/regression/test_White2004_4064-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4064-4/overview.txt +++ b/regression/test_White2004_4064-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4064-5/overview.txt b/regression/test_White2004_4064-5/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4064-5/overview.txt +++ b/regression/test_White2004_4064-5/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4065-1/overview.txt b/regression/test_White2004_4065-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4065-1/overview.txt +++ b/regression/test_White2004_4065-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4065-2/overview.txt b/regression/test_White2004_4065-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4065-2/overview.txt +++ b/regression/test_White2004_4065-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4065-3/overview.txt b/regression/test_White2004_4065-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4065-3/overview.txt +++ b/regression/test_White2004_4065-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4065-4/overview.txt b/regression/test_White2004_4065-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4065-4/overview.txt +++ b/regression/test_White2004_4065-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4065-5/overview.txt b/regression/test_White2004_4065-5/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4065-5/overview.txt +++ b/regression/test_White2004_4065-5/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4135-1/overview.txt b/regression/test_White2004_4135-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4135-1/overview.txt +++ b/regression/test_White2004_4135-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4135-2/overview.txt b/regression/test_White2004_4135-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4135-2/overview.txt +++ b/regression/test_White2004_4135-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4135-3/overview.txt b/regression/test_White2004_4135-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4135-3/overview.txt +++ b/regression/test_White2004_4135-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4136-1/overview.txt b/regression/test_White2004_4136-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4136-1/overview.txt +++ b/regression/test_White2004_4136-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4136-2/overview.txt b/regression/test_White2004_4136-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4136-2/overview.txt +++ b/regression/test_White2004_4136-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4136-3/overview.txt b/regression/test_White2004_4136-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4136-3/overview.txt +++ b/regression/test_White2004_4136-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4136-4/overview.txt b/regression/test_White2004_4136-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4136-4/overview.txt +++ b/regression/test_White2004_4136-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4140-1/overview.txt b/regression/test_White2004_4140-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4140-1/overview.txt +++ b/regression/test_White2004_4140-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4140-2/overview.txt b/regression/test_White2004_4140-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4140-2/overview.txt +++ b/regression/test_White2004_4140-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4162-1/overview.txt b/regression/test_White2004_4162-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4162-1/overview.txt +++ b/regression/test_White2004_4162-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4162-2/overview.txt b/regression/test_White2004_4162-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4162-2/overview.txt +++ b/regression/test_White2004_4162-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4162-3/overview.txt b/regression/test_White2004_4162-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4162-3/overview.txt +++ b/regression/test_White2004_4162-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4162-4/overview.txt b/regression/test_White2004_4162-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4162-4/overview.txt +++ b/regression/test_White2004_4162-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4163-1/overview.txt b/regression/test_White2004_4163-1/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4163-1/overview.txt +++ b/regression/test_White2004_4163-1/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4163-2/overview.txt b/regression/test_White2004_4163-2/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4163-2/overview.txt +++ b/regression/test_White2004_4163-2/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4163-3/overview.txt b/regression/test_White2004_4163-3/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4163-3/overview.txt +++ b/regression/test_White2004_4163-3/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/regression/test_White2004_4163-4/overview.txt b/regression/test_White2004_4163-4/overview.txt index b7537ac5..2d07fb26 100644 --- a/regression/test_White2004_4163-4/overview.txt +++ b/regression/test_White2004_4163-4/overview.txt @@ -1,6 +1,6 @@ Model Burnup : The local burnup is calculated from the fission rate density. Model Effective burnup : G. Khvostov et al., WRFPM-2005, Kyoto, Japan, 2005. -Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. +Model Grain growth : Ainscough et al., JNM, 49 (1973) 117-128. Model Gas production - Xe in UO2 Model Gas production - Kr in UO2 Model Gas production - He in UO2 @@ -12,11 +12,11 @@ Model Gas diffusion - Kr in UO2 Model Gas diffusion - He in UO2 Model Gas diffusion - Xe133 in UO2 Model Gas diffusion - Kr85m in UO2 -Model Grain-boundary micro-cracking from Barani et al. (2017), JNM +Model Grain-boundary micro-cracking : from Barani et al. (2017), JNM Model Intergranular bubble behavior : Pastore et al., NED, 256 (2013) 75-86. Matrix UO2 - : Ainscough et al., JNM, 49 (1973) 117-128. + Ainscough et al., JNM, 49 (1973) 117-128. iGrainBoundaryVacancyDiffusivity: from Reynolds and Burton, JNM, 82 (1979) 22-25. diff --git a/src/classes/Matrix.C b/src/classes/Matrix.C index 609fd3f2..83760b4b 100644 --- a/src/classes/Matrix.C +++ b/src/classes/Matrix.C @@ -22,7 +22,7 @@ void Matrix::setGrainBoundaryMobility(int input_value, SciantixArrayMassih A.R. (2018). UO2 Fuel Oxidation and Fission Gas Release, Swedish Radiation Safety Authority (SSM). * The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) * In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x)) * @@ -205,6 +204,8 @@ void Simulation::StoichiometryDeviation() */ case 5: { + reference += " : Massih, A. R. UO2 fuel oxidation and fission gas release. Swedish Radiation Safety Authority report, Report 2018 (2018): 25"; + double k_star = 1e4 * exp(-21253.0 / history_variable["Temperature"].getFinalValue() - 2.43); // (mol/m2 s) double tau_inv = k_star * (surface_to_volume) / 8.0e4; double s = 0.023; @@ -236,11 +237,11 @@ void Simulation::StoichiometryDeviation() /** * @brief The model for fuel oxidation and stoichimetry deviation evolution is described with a mechanistic Langmuir-based approach - * @ref Massih, A. R. "UO2 fuel oxidation and fission gas release." Swedish Radiation Safety Authority report, Report 2018 (2018): 25. + * @ref Massih A.R. (2018). UO2 Fuel Oxidation and Fission Gas Release, Swedish Radiation Safety Authority (SSM). * The oxidation rate follows: dx/dt = theta/tau (1 - sqrt(Po2(x)/Po2)) * In SCIANTIX, the ODE is rewritten as: dx / dt = K (1 - beta * exp(alpha * x)) * - * ### iStoichiometryDeviation = 5 + * ### iStoichiometryDeviation = 6 * * Range of utilization: * - Pure steam @@ -252,6 +253,8 @@ void Simulation::StoichiometryDeviation() */ case 6: { + reference += " : Massih, A. R. UO2 fuel oxidation and fission gas release. Swedish Radiation Safety Authority report, Report 2018 (2018): 25"; + surface_to_volume = 225; double k_star = 1e4 * exp(-21253.0 / history_variable["Temperature"].getFinalValue() - 2.43); // (mol/m2 s) From 0dce1ac8f6c5515adcc69e3a08cd0de5997ee4a8 Mon Sep 17 00:00:00 2001 From: giozu Date: Tue, 27 Aug 2024 17:56:49 +0200 Subject: [PATCH 06/15] Added instruction for pull request in BasicGuide.md --- utilities/BasicGuide.md | 50 ++++++++++++++++++++++++++++++++++++++++- 1 file changed, 49 insertions(+), 1 deletion(-) diff --git a/utilities/BasicGuide.md b/utilities/BasicGuide.md index 68407029..6f017167 100644 --- a/utilities/BasicGuide.md +++ b/utilities/BasicGuide.md @@ -106,7 +106,55 @@ Thank you for adhering to these guidelines! ## Useful Git Commands -Here are some helpful Git commands for managing your local and remote repositories: +Below are some essential Git commands for effectively managing your local and remote repositories: + +### How to Create a New Pull Request + +1. **Create and Switch to a New Branch:** + ```bash + git checkout -b new_repo + ``` + +2. **Make Changes and Commit Them:** + - Stage all changes: + ```bash + git add . + ``` + - Commit the changes: + ```bash + git commit -m "commit message" + ``` + - Push the new branch to the remote repository: + ```bash + git push origin new_repo + ``` + +3. **Create a New Pull Request:** + - Using GitHub CLI: + ```bash + gh pr create --base main --head new_repo --title "Title of the pull request" --body "Brief description of the pull request" + ``` + +4. **Check for Reviews or Approvals:** + - Ensure the pull request meets the necessary criteria. If the pull request is approved and ready to be merged, update your main branch: + ```bash + git pull origin main + ``` + +5. **Switch Back to the Main Branch:** + ```bash + git checkout main + ``` + +6. **Merge the New Branch into Main:** + ```bash + git merge new_repo + ``` + +7. **Push the Updated Main Branch to Complete the Pull Request:** + ```bash + git push -u origin main + ``` - **Delete old remote Git branches**: From ddd3130657d6811365dc8c86cb4c34581ac80f7a Mon Sep 17 00:00:00 2001 From: giozu Date: Tue, 27 Aug 2024 18:02:38 +0200 Subject: [PATCH 07/15] Added instruction for pull request in BasicGuide.md --- utilities/BasicGuide.md | 162 ++++++++++++++++++---------------------- 1 file changed, 73 insertions(+), 89 deletions(-) diff --git a/utilities/BasicGuide.md b/utilities/BasicGuide.md index 6f017167..98ed1625 100644 --- a/utilities/BasicGuide.md +++ b/utilities/BasicGuide.md @@ -1,31 +1,63 @@ # Basic guide -## Instructions for Committing New Code - -Follow these steps to commit new code to the SCIANTIX repository: - -1. Open your terminal and execute the following commands: +Open your terminal and execute the following commands to clone the code repository: ```bash gh repo clone sciantix/sciantix-official cd sciantix ``` -2. Create an issue on GitHub. +## Instructions for committing new code through a pull request -3. Proceed with the following commands: +Follow these steps to commit new code to the SCIANTIX repository: +1. **Create and switch to a new branch:** ```bash - git checkout -b - git add - git commit -m "" - git pull --rebase upstream version1.0 - git push origin + git checkout -b new_branch ``` -4. Create a merge request on GitHub. +2. **Make changes and commit them:** + - Stage all changes: + ```bash + git add . + ``` + - Commit the changes: + ```bash + git commit -m "commit message" + ``` + - Push the new branch to the remote repository: + ```bash + git push origin new_branch + ``` + +3. **Create a new pull request:** + - Using GitHub CLI: + ```bash + gh pr create --base main --head new_branch --title "Title of the pull request" --body "Brief description of the pull request" + ``` -### Check Your Work Status +4. **Check for reviews or approvals:** + - Ensure the pull request meets the necessary criteria. If the pull request is approved and ready to be merged, update your main branch: + ```bash + git pull origin main + ``` + +5. **Switch back to the main branch:** + ```bash + git checkout main + ``` + +6. **Merge the new branch into main:** + ```bash + git merge new_branch + ``` + +7. **Push the updated main branch to complete the pull request:** + ```bash + git push -u origin main + ``` + +### Check your work status At any time, you can check the status of your work by running: @@ -49,13 +81,13 @@ Follow these steps to build SCIANTIX on macOS: brew install git ``` -2. **Install Dependencies**: +2. **Install dependencies**: - Install CMake and g++ using Homebrew: ```bash brew install cmake g++ ``` -3. **Clone the Repository**: +3. **Clone the repository**: - Clone the repository: ```bash gh repo clone sciantix/sciantix-official @@ -75,87 +107,15 @@ cmake .. make -j ``` -5. **Locate the Executable**: +5. **Locate the executable**: - Find the `sciantix.x` executable in the `build` directory. --- -## Sciantix Syntax Guidelines - -To maintain consistency in the Sciantix codebase, please adhere to the following guidelines: - -- **Use extensive names** for functions and variables. Long names are encouraged for clarity. -- **Variable names** should be in lowercase with words separated by underscores (`_`). - - Example: `diffusion_coefficient` -- **Global variables** should be in uppercase with words separated by underscores (`_`). - - Example: `GAS_PRODUCED` -- **Input integer variables** (used for model selection) should start with an `i`. - - Example: `iGasDiffusivity` -- **Scaling factor variables** should start with `sf_`. - - Example: `sf_diffusion_coefficient` -- **Function names** should be in PascalCase with each word capitalized and no separation signs. - - Example: `HeliumDiffusionCoefficient` -- **File names** should match the name of the primary function they contain. -- **Documentation comments** in the code with `/**` are meant for inclusion in the Doxygen documentation and should be placed at the beginning of every function. -- **Regular comments** using `//` should be added liberally throughout the code. -- **Scientific references** should be added as comments in the code wherever applicable (e.g., parameter values, equations). - -Thank you for adhering to these guidelines! - ---- - ## Useful Git Commands Below are some essential Git commands for effectively managing your local and remote repositories: -### How to Create a New Pull Request - -1. **Create and Switch to a New Branch:** - ```bash - git checkout -b new_repo - ``` - -2. **Make Changes and Commit Them:** - - Stage all changes: - ```bash - git add . - ``` - - Commit the changes: - ```bash - git commit -m "commit message" - ``` - - Push the new branch to the remote repository: - ```bash - git push origin new_repo - ``` - -3. **Create a New Pull Request:** - - Using GitHub CLI: - ```bash - gh pr create --base main --head new_repo --title "Title of the pull request" --body "Brief description of the pull request" - ``` - -4. **Check for Reviews or Approvals:** - - Ensure the pull request meets the necessary criteria. If the pull request is approved and ready to be merged, update your main branch: - ```bash - git pull origin main - ``` - -5. **Switch Back to the Main Branch:** - ```bash - git checkout main - ``` - -6. **Merge the New Branch into Main:** - ```bash - git merge new_repo - ``` - -7. **Push the Updated Main Branch to Complete the Pull Request:** - ```bash - git push -u origin main - ``` - - **Delete old remote Git branches**: ```bash @@ -192,4 +152,28 @@ Below are some essential Git commands for effectively managing your local and re --- +## Sciantix syntax guidelines + +To maintain consistency in the Sciantix codebase, please adhere to the following guidelines: + +- **Use extensive names** for functions and variables. Long names are encouraged for clarity. +- **Variable names** should be in lowercase with words separated by underscores (`_`). + - Example: `diffusion_coefficient` +- **Global variables** should be in uppercase with words separated by underscores (`_`). + - Example: `GAS_PRODUCED` +- **Input integer variables** (used for model selection) should start with an `i`. + - Example: `iGasDiffusivity` +- **Scaling factor variables** should start with `sf_`. + - Example: `sf_diffusion_coefficient` +- **Function names** should be in PascalCase with each word capitalized and no separation signs. + - Example: `HeliumDiffusionCoefficient` +- **File names** should match the name of the primary function they contain. +- **Documentation comments** in the code with `/**` are meant for inclusion in the Doxygen documentation and should be placed at the beginning of every function. +- **Regular comments** using `//` should be added liberally throughout the code. +- **Scientific references** should be added as comments in the code wherever applicable (e.g., parameter values, equations). + +Thank you for adhering to these guidelines! + +--- + We hope this guide helps simplify the process of committing new code and building SCIANTIX on macOS, while also ensuring consistency in the source code through our syntax guidelines. If you encounter any issues or have suggestions, please feel free to contact the developers. \ No newline at end of file From 4c65289a615d2322d4490ad6e6e7d8886dfa75e1 Mon Sep 17 00:00:00 2001 From: giozu Date: Tue, 27 Aug 2024 18:04:50 +0200 Subject: [PATCH 08/15] Added instruction for pull request in BasicGuide.md --- utilities/BasicGuide.md | 8 +------- 1 file changed, 1 insertion(+), 7 deletions(-) diff --git a/utilities/BasicGuide.md b/utilities/BasicGuide.md index 98ed1625..f0d69b2e 100644 --- a/utilities/BasicGuide.md +++ b/utilities/BasicGuide.md @@ -1,12 +1,5 @@ # Basic guide -Open your terminal and execute the following commands to clone the code repository: - - ```bash - gh repo clone sciantix/sciantix-official - cd sciantix - ``` - ## Instructions for committing new code through a pull request Follow these steps to commit new code to the SCIANTIX repository: @@ -62,6 +55,7 @@ Follow these steps to commit new code to the SCIANTIX repository: At any time, you can check the status of your work by running: ```bash +git fetch git status ``` From 147c55b9285686d49514b44458544727a1527b8b Mon Sep 17 00:00:00 2001 From: giozu Date: Tue, 27 Aug 2024 19:07:32 +0200 Subject: [PATCH 09/15] update files in utilities --- utilities/BasicGuide.md | 6 +- utilities/MMS_verification/mms_Decay.py | 4 +- utilities/MMS_verification/mms_Integrator.py | 2 +- .../spectral_diffusion_algorithm.py | 8 ++ utilities/postProcessing/output.txt | 102 ------------------ utilities/solid_fp_swelling.py | 3 + 6 files changed, 17 insertions(+), 108 deletions(-) delete mode 100644 utilities/postProcessing/output.txt diff --git a/utilities/BasicGuide.md b/utilities/BasicGuide.md index f0d69b2e..e0c4637a 100644 --- a/utilities/BasicGuide.md +++ b/utilities/BasicGuide.md @@ -1,5 +1,7 @@ # Basic guide +We hope this guide helps simplify the process of committing new code and building SCIANTIX, while also ensuring consistency in the source code through our syntax guidelines. If you encounter any issues or have suggestions, please feel free to contact the developers. + ## Instructions for committing new code through a pull request Follow these steps to commit new code to the SCIANTIX repository: @@ -168,6 +170,4 @@ To maintain consistency in the Sciantix codebase, please adhere to the following Thank you for adhering to these guidelines! ---- - -We hope this guide helps simplify the process of committing new code and building SCIANTIX on macOS, while also ensuring consistency in the source code through our syntax guidelines. If you encounter any issues or have suggestions, please feel free to contact the developers. \ No newline at end of file +--- \ No newline at end of file diff --git a/utilities/MMS_verification/mms_Decay.py b/utilities/MMS_verification/mms_Decay.py index ebc4135e..6685fa71 100644 --- a/utilities/MMS_verification/mms_Decay.py +++ b/utilities/MMS_verification/mms_Decay.py @@ -1,9 +1,9 @@ """ This script performs the numerical verification via method of manufactured solution (MMS) of the -SCIANTIX solver "NewtonBlackburn" +SCIANTIX solver "Decay" Author: G. Zullo -Ref: Oberkampf , W. L., Trucano , T. G., and Hirsch , C. (December 21, 2004). "Verification, validation, and predictive capability in computational engineering and physics." ASME. Appl. Mech. Rev. September 2004; 57(5): 345–384. https://doi.org/10.1115/1.1767847 +Ref: Oberkampf , W. L., Trucano , T. G., and Hirsch , C. (December 21, 2004). "Verification, validation, and predictive capability in computational engineering and physics." ASME. Appl. Mech. Rev. September 2004; 57(5): 345-384. https://doi.org/10.1115/1.1767847 """ diff --git a/utilities/MMS_verification/mms_Integrator.py b/utilities/MMS_verification/mms_Integrator.py index d9a46d9e..cf7d99a9 100644 --- a/utilities/MMS_verification/mms_Integrator.py +++ b/utilities/MMS_verification/mms_Integrator.py @@ -1,6 +1,6 @@ """ This script performs the numerical verification via method of manufactured solution (MMS) of the -SCIANTIX solver "NewtonBlackburn" +SCIANTIX solver "Integrator" Author: G. Zullo Ref: Oberkampf , W. L., Trucano , T. G., and Hirsch , C. (December 21, 2004). "Verification, validation, and predictive capability in computational engineering and physics." ASME. Appl. Mech. Rev. September 2004; 57(5): 345–384. https://doi.org/10.1115/1.1767847 diff --git a/utilities/MMS_verification/spectral_diffusion_algorithm.py b/utilities/MMS_verification/spectral_diffusion_algorithm.py index 20d2992e..e228f3fc 100644 --- a/utilities/MMS_verification/spectral_diffusion_algorithm.py +++ b/utilities/MMS_verification/spectral_diffusion_algorithm.py @@ -1,3 +1,11 @@ +""" +This script is the equivalent of the SCIANTIX solver SpectralDiffusion2equations in Solver.C/h. +It can be used for testing purposes. + +Author: G. Zullo + +""" + import math import numpy as np import matplotlib.pyplot as plt diff --git a/utilities/postProcessing/output.txt b/utilities/postProcessing/output.txt deleted file mode 100644 index 79fb01b1..00000000 --- a/utilities/postProcessing/output.txt +++ /dev/null @@ -1,102 +0,0 @@ -Time (h) Temperature (K) Fission rate (fiss / m3 s) Hydrostatic stress (MPa) Grain radius (m) Xe produced (at/m3) Xe in grain (at/m3) Xe in intragranular solution (at/m3) Xe in intragranular bubbles (at/m3) Xe at grain boundary (at/m3) Xe released (at/m3) Kr produced (at/m3) Kr in grain (at/m3) Kr in intragranular solution (at/m3) Kr in intragranular bubbles (at/m3) Kr at grain boundary (at/m3) Kr released (at/m3) Fission gas release (/) Intragranular bubble concentration (bub/m3) Intragranular bubble radius (m) Intragranular gas bubble swelling (/) Intergranular bubble concentration (bub/m2) Intergranular atoms per bubble (at/bub) Intergranular vacancies per bubble (vac/bub) Intergranular bubble radius (m) Intergranular bubble area (m2) Intergranular bubble volume (m3) Intergranular fractional coverage (/) Intergranular saturation fractional coverage (/) Intergranular gas swelling (/) Intergranular fractional intactness (/) Burnup (MWd/kgUO2) U235 (at/m3) U238 (at/m3) -0 1273 1e+19 0 5e-06 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 4e+13 0 0 0 0 0 0 0.5 0 1 0 7.43262e+26 2.372858e+28 -55 1273 1e+19 0 5e-06 4.752e+23 4.490564e+23 4.490564e+23 0 2.61436e+22 0 5.94e+22 5.613205e+22 5.613205e+22 0 3.26795e+21 0 0 1.308758e+24 0 0 3.976259e+13 1232.798 1981.221 6.375315e-09 7.493094e-17 1.830117e-25 0.002979448 0.5 4.366212e-06 1 0.06517776 7.43262e+26 2.372858e+28 -110 1273 1e+19 0 5e-06 9.504e+23 8.92326e+23 6.411603e+23 2.511657e+23 5.807396e+22 0 1.188e+23 1.115408e+23 8.014504e+22 3.139572e+22 7.259245e+21 0 0 1.326059e+24 0 0 3.954566e+13 2753.493 6405.957 8.851333e-09 1.444359e-16 4.897787e-25 0.005711812 0.5 1.162117e-05 1 0.1303555 7.43262e+26 2.372858e+28 -165 1273 1e+19 0 5e-06 1.4256e+24 1.327414e+24 9.502471e+23 3.771673e+23 9.818556e+22 0 1.782e+23 1.659268e+23 1.187809e+23 4.714591e+22 1.227319e+22 0 0 1.326288e+24 1.276546e-10 1.155676e-05 3.929507e+13 4685.014 13966.11 1.107252e-08 2.260222e-16 9.587688e-25 0.008881558 0.5 2.260493e-05 1 0.1955333 7.43262e+26 2.372858e+28 -220 1273 1e+19 0 5e-06 1.9008e+24 1.757899e+24 1.170399e+24 5.874995e+23 1.429014e+23 0 2.376e+23 2.197373e+23 1.462999e+23 7.343744e+22 1.786267e+22 0 0 1.045959e+24 1.582227e-10 1.735441e-05 3.902655e+13 6865.584 24683.21 1.307164e-08 3.150052e-16 1.57748e-24 0.01229357 0.5 3.693816e-05 1 0.260711 7.43262e+26 2.372858e+28 -275 1273 1e+19 0 5e-06 2.376e+24 2.18037e+24 1.547218e+24 6.331519e+23 1.956298e+23 0 2.97e+23 2.725463e+23 1.934023e+23 7.914398e+22 2.445372e+22 0 0 9.892441e+23 1.868517e-10 2.703232e-05 3.872441e+13 9472.213 39612.61 1.504192e-08 4.171231e-16 2.403718e-24 0.01615285 0.5 5.584954e-05 1 0.3258888 7.43262e+26 2.372858e+28 -330 1273 1e+19 0 5e-06 2.8512e+24 2.597456e+24 1.858989e+24 7.384667e+23 2.537439e+23 0 3.564e+23 3.24682e+23 2.323737e+23 9.230833e+22 3.171799e+22 0 0 9.420048e+23 1.947215e-10 2.91329e-05 3.839918e+13 12390.11 58983.72 1.694666e-08 5.294515e-16 3.437371e-24 0.0203305 0.5 7.919534e-05 1 0.3910665 7.43262e+26 2.372858e+28 -385 1273 1e+19 0 5e-06 3.3264e+24 3.009399e+24 2.179607e+24 8.297922e+23 3.170012e+23 0 4.158e+23 3.761748e+23 2.724508e+23 1.03724e+23 3.962516e+22 0 0 9.293112e+23 2.058981e-10 3.39787e-05 3.805324e+13 15619.63 83192.6 1.880227e-08 6.517461e-16 4.694668e-24 0.02480105 0.5 0.0001071884 1 0.4562443 7.43262e+26 2.372858e+28 -440 1273 1e+19 0 5e-06 3.8016e+24 3.417023e+24 2.478209e+24 9.388148e+23 3.845766e+23 0 4.752e+23 4.271279e+23 3.097761e+23 1.173518e+23 4.807208e+22 0 0 9.122055e+23 2.153879e-10 3.818081e-05 3.769061e+13 19131.59 112497.1 2.061068e-08 7.831456e-16 6.183737e-24 0.02951724 0.5 0.0001398413 1 0.5214221 7.43262e+26 2.372858e+28 -495 1273 1e+19 0 5e-06 4.2768e+24 3.82049e+24 2.779704e+24 1.040787e+24 4.563098e+23 0 5.346e+23 4.775613e+23 3.47463e+23 1.300983e+23 5.703872e+22 0 0 8.979899e+23 2.256136e-10 4.319722e-05 3.731276e+13 22929.98 147281.5 2.238353e-08 9.236663e-16 7.920633e-24 0.03446455 0.5 0.0001773244 1 0.5865998 7.43262e+26 2.372858e+28 -550 1273 1e+19 0 5e-06 4.752e+24 4.22007e+24 3.077699e+24 1.142371e+24 5.319299e+23 0 5.94e+23 5.275088e+23 3.847124e+23 1.427963e+23 6.649124e+22 0 0 8.830742e+23 2.348104e-10 4.788919e-05 3.69212e+13 27013.44 187939.6 2.41286e-08 1.073302e-15 9.92134e-24 0.03962761 0.5 0.0002197847 1 0.6517776 7.43262e+26 2.372858e+28 -605 1273 1e+19 0 5e-06 5.2272e+24 4.615921e+24 3.376219e+24 1.239702e+24 6.112788e+23 0 6.534e+23 5.769902e+23 4.220274e+23 1.549628e+23 7.640984e+22 0 0 8.699533e+23 2.434255e-10 5.256333e-05 3.6517e+13 31386.69 234914.7 2.585318e-08 1.232213e-15 1.220439e-23 0.04499672 0.5 0.0002674005 1 0.7169553 7.43262e+26 2.372858e+28 -660 1273 1e+19 0 5e-06 5.7024e+24 5.008231e+24 3.67268e+24 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1.660766e+08 2.14903e-07 8.514177e-14 7.009728e-21 0.5 0.5 0.02469902 1 5.409754 7.43262e+26 2.372858e+28 -4620 1273 1e+19 0 5e-06 3.99168e+25 2.783375e+25 2.183306e+25 6.000689e+24 8.242267e+24 3.840788e+24 4.9896e+24 3.479218e+24 2.729132e+24 7.500861e+23 1.030283e+24 4.800985e+23 0.09621983 6.111938e+23 4.747334e-10 0.0002739157 5.661894e+12 2729520 1.755202e+08 2.188645e-07 8.830968e-14 7.404567e-21 0.5 0.5 0.02515432 1 5.474932 7.43262e+26 2.372858e+28 -4675 1273 1e+19 0 5e-06 4.0392e+25 2.809873e+25 2.205073e+25 6.047998e+24 8.261888e+24 4.031382e+24 5.049e+24 3.512341e+24 2.756342e+24 7.559997e+23 1.032736e+24 5.039227e+23 0.09980644 6.098426e+23 4.763471e-10 0.0002761067 5.459008e+12 2837702 1.854872e+08 2.228944e-07 9.159172e-14 7.821167e-21 0.5 0.5 0.02561749 1 5.540109 7.43262e+26 2.372858e+28 -4730 1273 1e+19 0 5e-06 4.08672e+25 2.836263e+25 2.226763e+25 6.095001e+24 8.282416e+24 4.222156e+24 5.1084e+24 3.545329e+24 2.783453e+24 7.618751e+23 1.035302e+24 5.277694e+23 0.103314 6.085101e+23 4.77944e-10 0.0002782835 5.263686e+12 2950315 1.960015e+08 2.269923e-07 9.499048e-14 8.260518e-21 0.5 0.5 0.02608846 1 5.605287 7.43262e+26 2.372858e+28 -4785 1273 1e+19 0 5e-06 4.13424e+25 2.862545e+25 2.248375e+25 6.141702e+24 8.303902e+24 4.41305e+24 5.1678e+24 3.578181e+24 2.810468e+24 7.677128e+23 1.037988e+24 5.516313e+23 0.1067439 6.071957e+23 4.795245e-10 0.0002804462 5.075709e+12 3067516 2.070874e+08 2.311574e-07 9.850841e-14 8.723628e-21 0.5 0.5 0.02656716 1 5.670465 7.43262e+26 2.372858e+28 -4840 1273 1e+19 0 5e-06 4.18176e+25 2.88872e+25 2.269909e+25 6.188106e+24 8.326396e+24 4.604007e+24 5.2272e+24 3.6109e+24 2.837386e+24 7.735132e+23 1.0408e+24 5.755009e+23 0.1100973 6.058991e+23 4.810888e-10 0.0002825951 4.894864e+12 3189464 2.187697e+08 2.353888e-07 1.021479e-13 9.21152e-21 0.5 0.5 0.02705348 1 5.735643 7.43262e+26 2.372858e+28 -4895 1273 1e+19 0 5e-06 4.22928e+25 2.914788e+25 2.291367e+25 6.234215e+24 8.349949e+24 4.794967e+24 5.2866e+24 3.643485e+24 2.864209e+24 7.792768e+23 1.043744e+24 5.993708e+23 0.1133755 6.046197e+23 4.826373e-10 0.0002847302 4.720937e+12 3316324 2.310733e+08 2.396856e-07 1.059112e-13 9.725231e-21 0.5 0.5 0.02754732 1 5.80082 7.43262e+26 2.372858e+28 -4950 1273 1e+19 0 5e-06 4.2768e+25 2.940752e+25 2.312748e+25 6.280033e+24 8.374612e+24 4.985871e+24 5.346e+24 3.67594e+24 2.890935e+24 7.850041e+23 1.046827e+24 6.232339e+23 0.1165795 6.033573e+23 4.841703e-10 0.0002868518 4.553717e+12 3448260 2.440235e+08 2.440468e-07 1.098004e-13 1.026581e-20 0.5 0.5 0.02804855 1 5.865998 7.43262e+26 2.372858e+28 -5005 1273 1e+19 0 5e-06 4.32432e+25 2.96661e+25 2.334054e+25 6.325563e+24 8.400436e+24 5.176661e+24 5.4054e+24 3.708263e+24 2.917568e+24 7.906954e+23 1.050054e+24 6.470826e+23 0.1197104 6.021115e+23 4.85688e-10 0.00028896 4.392995e+12 3585439 2.576458e+08 2.48471e-07 1.138176e-13 1.083431e-20 0.5 0.5 0.02855703 1 5.931176 7.43262e+26 2.372858e+28 -5060 1273 1e+19 0 5e-06 4.37184e+25 2.992365e+25 2.355284e+25 6.37081e+24 8.427468e+24 5.36728e+24 5.4648e+24 3.740456e+24 2.944105e+24 7.963513e+23 1.053434e+24 6.7091e+23 0.1227694 6.008818e+23 4.871909e-10 0.000291055 4.238564e+12 3728033 2.719657e+08 2.52957e-07 1.179645e-13 1.143179e-20 0.5 0.5 0.02907262 1 5.996354 7.43262e+26 2.372858e+28 -5115 1273 1e+19 0 5e-06 4.41936e+25 3.018017e+25 2.376439e+25 6.415776e+24 8.45576e+24 5.55767e+24 5.5242e+24 3.772521e+24 2.970549e+24 8.01972e+23 1.05697e+24 6.947088e+23 0.1257574 5.996679e+23 4.88679e-10 0.0002931369 4.090218e+12 3876211 2.870089e+08 2.575033e-07 1.222429e-13 1.205931e-20 0.5 0.5 0.02959513 1 6.061531 7.43262e+26 2.372858e+28 -5170 1273 1e+19 0 5e-06 4.46688e+25 3.043566e+25 2.39752e+25 6.460465e+24 8.485358e+24 5.747778e+24 5.5836e+24 3.804458e+24 2.9969e+24 8.075581e+23 1.06067e+24 7.184722e+23 0.1286754 5.984695e+23 4.901528e-10 0.0002952059 3.947756e+12 4030149 3.028009e+08 2.621084e-07 1.266542e-13 1.271794e-20 0.5 0.5 0.03012439 1 6.126709 7.43262e+26 2.372858e+28 -5225 1273 1e+19 0 5e-06 4.5144e+25 3.069014e+25 2.418526e+25 6.504879e+24 8.516308e+24 5.937548e+24 5.643e+24 3.836268e+24 3.023158e+24 8.131099e+23 1.064539e+24 7.421935e+23 0.1315246 5.972862e+23 4.916124e-10 0.0002972621 3.810977e+12 4190022 3.193673e+08 2.667706e-07 1.311999e-13 1.340873e-20 0.5 0.5 0.03066022 1 6.191887 7.43262e+26 2.372858e+28 -5280 1273 1e+19 0 5e-06 4.56192e+25 3.094361e+25 2.439459e+25 6.549023e+24 8.548657e+24 6.126929e+24 5.7024e+24 3.867952e+24 3.049324e+24 8.186278e+23 1.068582e+24 7.658661e+23 0.1343059 5.961177e+23 4.930582e-10 0.0002993058 3.679686e+12 4356005 3.367333e+08 2.714881e-07 1.358812e-13 1.413273e-20 0.5 0.5 0.03120241 1 6.257065 7.43262e+26 2.372858e+28 -5335 1273 1e+19 0 5e-06 4.60944e+25 3.119608e+25 2.460319e+25 6.592898e+24 8.582445e+24 6.31587e+24 5.7618e+24 3.899511e+24 3.075398e+24 8.241123e+23 1.072806e+24 7.894838e+23 0.1370203 5.949637e+23 4.944903e-10 0.0003013369 3.553687e+12 4528279 3.549241e+08 2.76259e-07 1.406989e-13 1.489099e-20 0.5 0.5 0.03175074 1 6.322242 7.43262e+26 2.372858e+28 -5390 1273 1e+19 0 5e-06 4.65696e+25 3.144756e+25 2.481105e+25 6.636509e+24 8.617715e+24 6.504324e+24 5.8212e+24 3.930945e+24 3.101381e+24 8.295636e+23 1.077214e+24 8.130405e+23 0.1396689 5.938239e+23 4.95909e-10 0.0003033557 3.432791e+12 4707020 3.739644e+08 2.810816e-07 1.456541e-13 1.568452e-20 0.5 0.5 0.032305 1 6.38742 7.43262e+26 2.372858e+28 -5445 1273 1e+19 0 5e-06 4.70448e+25 3.169805e+25 2.501819e+25 6.679857e+24 8.654505e+24 6.692245e+24 5.8806e+24 3.962256e+24 3.127274e+24 8.349822e+23 1.081813e+24 8.365306e+23 0.1422526 5.92698e+23 4.973145e-10 0.0003053624 3.316811e+12 4892410 3.938784e+08 2.859537e-07 1.507472e-13 1.651434e-20 0.5 0.5 0.03286496 1 6.452598 7.43262e+26 2.372858e+28 -5500 1273 1e+19 0 5e-06 4.752e+25 3.194756e+25 2.522461e+25 6.722947e+24 8.692852e+24 6.879589e+24 5.94e+24 3.993445e+24 3.153077e+24 8.403683e+23 1.086606e+24 8.599486e+23 0.1447725 5.915857e+23 4.987071e-10 0.0003073569 3.205562e+12 5084630 4.146903e+08 2.908734e-07 1.559789e-13 1.738145e-20 0.5 0.5 0.03343038 1 6.517776 7.43262e+26 2.372858e+28 diff --git a/utilities/solid_fp_swelling.py b/utilities/solid_fp_swelling.py index 1faba253..b314ee97 100644 --- a/utilities/solid_fp_swelling.py +++ b/utilities/solid_fp_swelling.py @@ -1,3 +1,6 @@ +# Brief script to compute the correlation term between burnup and swelling due to solid fission products +# Author: G. Zullo + import numpy as np # Olander 1976 - Formula for swelling due to solid FPs From 477f45566ab8d23a6d42eeab10641a3461e7815b Mon Sep 17 00:00:00 2001 From: giozu Date: Wed, 28 Aug 2024 10:38:57 +0200 Subject: [PATCH 10/15] updated plotting files --- .../print_input_initial_conditions.py | 3 +- .../print_input_scaling_factors.py | 3 +- .../inputExample/print_input_settings.py | 2 +- utilities/postProcessing/output.txt | 102 +++ utilities/postProcessing/sciantix.py | 606 ------------------ utilities/postProcessing/sciantix_gui.py | 192 ++++++ utilities/postProcessing/sciantix_plot.py | 215 +++++++ 7 files changed, 514 insertions(+), 609 deletions(-) create mode 100644 utilities/postProcessing/output.txt delete mode 100644 utilities/postProcessing/sciantix.py create mode 100644 utilities/postProcessing/sciantix_gui.py create mode 100644 utilities/postProcessing/sciantix_plot.py diff --git a/utilities/inputExample/print_input_initial_conditions.py b/utilities/inputExample/print_input_initial_conditions.py index dada7c5d..0bd2658c 100644 --- a/utilities/inputExample/print_input_initial_conditions.py +++ b/utilities/inputExample/print_input_initial_conditions.py @@ -1,7 +1,8 @@ """ -@author (G. Zullo) This is a python script to write the SCIANTIX default input file "input_initial_conditions.txt". +@author G. Zullo + """ with open('input_initial_conditions.txt', 'w') as file: diff --git a/utilities/inputExample/print_input_scaling_factors.py b/utilities/inputExample/print_input_scaling_factors.py index 7990f05f..b0a19bca 100644 --- a/utilities/inputExample/print_input_scaling_factors.py +++ b/utilities/inputExample/print_input_scaling_factors.py @@ -1,7 +1,8 @@ """ -@author (G. Zullo) This is a python script to write the SCIANTIX optional input file "input_scaling_factors.txt". +@author G. Zullo + """ with open('input_scaling_factors.txt', 'w') as file: diff --git a/utilities/inputExample/print_input_settings.py b/utilities/inputExample/print_input_settings.py index 46a3401a..d3a1b3e9 100644 --- a/utilities/inputExample/print_input_settings.py +++ b/utilities/inputExample/print_input_settings.py @@ -1,6 +1,6 @@ """ -@author (G. Zullo) This is a python script to write the SCIANTIX default input file "input_settings.txt". +@author G. Zullo """ diff --git a/utilities/postProcessing/output.txt b/utilities/postProcessing/output.txt new file mode 100644 index 00000000..0f38ab83 --- /dev/null +++ b/utilities/postProcessing/output.txt @@ -0,0 +1,102 @@ +Time (h) Temperature (K) Fission rate (fiss / m3 s) Hydrostatic stress (MPa) Grain radius (m) Xe produced (at/m3) Xe in grain (at/m3) Xe in intragranular solution (at/m3) Xe in intragranular bubbles (at/m3) Xe at grain boundary (at/m3) Xe released (at/m3) Kr produced (at/m3) Kr in grain (at/m3) Kr in intragranular solution (at/m3) Kr in intragranular bubbles (at/m3) Kr at grain boundary (at/m3) Kr released (at/m3) Fission gas release (/) Intragranular bubble concentration (bub/m3) Intragranular bubble radius (m) Intragranular gas bubble swelling (/) Intergranular bubble concentration (bub/m2) Intergranular atoms per bubble (at/bub) Intergranular vacancies per bubble (vac/bub) Intergranular bubble radius (m) Intergranular bubble area (m2) Intergranular bubble volume (m3) Intergranular fractional coverage (/) Intergranular saturation fractional coverage (/) Intergranular gas swelling (/) Intergranular fractional intactness (/) Burnup (MWd/kgUO2) U235 (at/m3) U238 (at/m3) +0 1273 1e+19 0 5e-06 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 2e+13 0 0 0 0 0 0 0.5 0 1 0 7.209709e+26 2.301694e+28 +55 1273 1e+19 0 5e-06 4.752e+23 4.490564e+23 4.490564e+23 0 2.61436e+22 0 5.94e+22 5.613205e+22 5.613205e+22 0 3.26795e+21 0 0 1.308758e+24 0 0 1.996233e+13 2455.587 4971.974 8.318091e-09 1.275572e-16 4.064853e-25 0.00254634 0.5 4.868638e-06 1 0.06719293 7.209709e+26 2.301694e+28 +110 1273 1e+19 0 5e-06 9.504e+23 8.92326e+23 6.411603e+23 2.511657e+23 5.807396e+22 0 1.188e+23 1.115408e+23 8.014504e+22 3.139572e+22 7.259245e+21 0 0 1.326059e+24 0 0 1.990252e+13 5471.1 16371.28 1.166885e-08 2.51023e-16 1.122167e-24 0.004995991 0.5 1.340037e-05 1 0.1343859 7.209709e+26 2.301694e+28 +165 1273 1e+19 0 5e-06 1.4256e+24 1.327414e+24 9.502471e+23 3.771673e+23 9.818556e+22 0 1.782e+23 1.659268e+23 1.187809e+23 4.714591e+22 1.227319e+22 0 0 1.326288e+24 1.276546e-10 1.155676e-05 1.982226e+13 9287.435 36096.01 1.470241e-08 3.985061e-16 2.244604e-24 0.007899291 0.5 2.669587e-05 1 0.2015788 7.209709e+26 2.301694e+28 +220 1273 1e+19 0 5e-06 1.9008e+24 1.757899e+24 1.170399e+24 5.874995e+23 1.429014e+23 0 2.376e+23 2.197373e+23 1.462999e+23 7.343744e+22 1.786267e+22 0 0 1.045959e+24 1.582227e-10 1.735441e-05 1.972783e+13 13581.83 64301.61 1.745095e-08 5.614305e-16 3.753455e-24 0.01107581 0.5 4.442851e-05 1 0.2687717 7.209709e+26 2.301694e+28 +275 1273 1e+19 0 5e-06 2.376e+24 2.18037e+24 1.547218e+24 6.331519e+23 1.956298e+23 0 2.97e+23 2.725463e+23 1.934023e+23 7.914398e+22 2.445372e+22 0 0 9.892441e+23 1.868517e-10 2.703232e-05 1.961608e+13 18699.24 103666.5 2.01599e-08 7.492631e-16 5.786803e-24 0.0146976 0.5 6.810863e-05 1 0.3359647 7.209709e+26 2.301694e+28 +330 1273 1e+19 0 5e-06 2.8512e+24 2.597456e+24 1.858989e+24 7.384667e+23 2.537439e+23 0 3.564e+23 3.24682e+23 2.323737e+23 9.230833e+22 3.171799e+22 0 0 9.420048e+23 1.947215e-10 2.91329e-05 1.949037e+13 24410.51 154837.6 2.278286e-08 9.569167e-16 8.352152e-24 0.01865066 0.5 9.76719e-05 1 0.4031576 7.209709e+26 2.301694e+28 +385 1273 1e+19 0 5e-06 3.3264e+24 3.009399e+24 2.179607e+24 8.297922e+23 3.170012e+23 0 4.158e+23 3.761748e+23 2.724508e+23 1.03724e+23 3.962516e+22 0 0 9.293112e+23 2.058981e-10 3.39787e-05 1.935226e+13 30713.58 218814.6 2.533872e-08 1.183661e-15 1.149021e-23 0.02290652 0.5 0.000133417 1 0.4703505 7.209709e+26 2.301694e+28 +440 1273 1e+19 0 5e-06 3.8016e+24 3.417023e+24 2.478209e+24 9.388148e+23 3.845766e+23 0 4.752e+23 4.271279e+23 3.097761e+23 1.173518e+23 4.807208e+22 0 0 9.122055e+23 2.153879e-10 3.818081e-05 1.92037e+13 37549.07 296231 2.78291e-08 1.427763e-15 1.522199e-23 0.02741834 0.5 0.0001753911 1 0.5375435 7.209709e+26 2.301694e+28 +495 1273 1e+19 0 5e-06 4.2768e+24 3.82049e+24 2.779704e+24 1.040787e+24 4.563098e+23 0 5.346e+23 4.775613e+23 3.47463e+23 1.300983e+23 5.703872e+22 0 0 8.979899e+23 2.256136e-10 4.319722e-05 1.904569e+13 44922.54 388025.7 3.026866e-08 1.689056e-15 1.958634e-23 0.03216924 0.5 0.0002238213 1 0.6047364 7.209709e+26 2.301694e+28 +550 1273 1e+19 0 5e-06 4.752e+24 4.22007e+24 3.077699e+24 1.142371e+24 5.319299e+23 0 5.94e+23 5.275088e+23 3.847124e+23 1.427963e+23 6.649124e+22 0 0 8.830742e+23 2.348104e-10 4.788919e-05 1.887911e+13 52829.21 495160 3.266763e-08 1.967402e-15 2.462219e-23 0.0371428 0.5 0.0002789071 1 0.6719293 7.209709e+26 2.301694e+28 +605 1273 1e+19 0 5e-06 5.2272e+24 4.615921e+24 3.376219e+24 1.239702e+24 6.112788e+23 0 6.534e+23 5.769902e+23 4.220274e+23 1.549628e+23 7.640984e+22 0 0 8.699533e+23 2.434255e-10 5.256333e-05 1.870464e+13 61276.11 618717.3 3.503575e-08 2.26298e-15 3.037443e-23 0.04232822 0.5 0.0003408857 1 0.7391223 7.209709e+26 2.301694e+28 +660 1273 1e+19 0 5e-06 5.7024e+24 5.008231e+24 3.67268e+24 1.335551e+24 6.941688e+23 0 7.128e+23 6.260289e+23 4.59085e+23 1.669439e+23 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2.355284e+25 6.37081e+24 8.889484e+24 4.905264e+24 5.4648e+24 3.740456e+24 2.944105e+24 7.963513e+23 1.111186e+24 6.13158e+23 0.1122014 6.008818e+23 4.871909e-10 0.000291055 2.610056e+12 6385988 5.655053e+08 3.223526e-07 1.915668e-13 2.365743e-20 0.5 0.5 0.03704832 1 6.18175 7.209709e+26 2.301694e+28 +5115 1273 1e+19 0 5e-06 4.41936e+25 3.018017e+25 2.376439e+25 6.415776e+24 8.934607e+24 5.078823e+24 5.5242e+24 3.772521e+24 2.970549e+24 8.01972e+23 1.116826e+24 6.348529e+23 0.1149221 5.996679e+23 4.88679e-10 0.0002931369 2.532294e+12 6615499 5.918878e+08 3.272646e-07 1.974494e-13 2.475546e-20 0.5 0.5 0.03761286 1 6.248943 7.209709e+26 2.301694e+28 +5170 1273 1e+19 0 5e-06 4.46688e+25 3.043566e+25 2.39752e+25 6.460465e+24 8.981305e+24 5.25183e+24 5.5836e+24 3.804458e+24 2.9969e+24 8.075581e+23 1.122663e+24 6.564788e+23 0.1175727 5.984695e+23 4.901528e-10 0.0002952059 2.457463e+12 6852575 6.192639e+08 3.3221e-07 2.034619e-13 2.589476e-20 0.5 0.5 0.03818124 1 6.316136 7.209709e+26 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2.222728e-13 2.956765e-20 0.5 0.5 0.03990723 1 6.517715 7.209709e+26 2.301694e+28 +5390 1273 1e+19 0 5e-06 4.65696e+25 3.144756e+25 2.481105e+25 6.636509e+24 9.184127e+24 5.937912e+24 5.8212e+24 3.930945e+24 3.101381e+24 8.295636e+23 1.148016e+24 7.42239e+23 0.1275062 5.938239e+23 4.95909e-10 0.0003033557 2.185329e+12 7879931 7.390569e+08 3.522879e-07 2.287985e-13 3.087927e-20 0.5 0.5 0.04048882 1 6.584907 7.209709e+26 2.301694e+28 +5445 1273 1e+19 0 5e-06 4.70448e+25 3.169805e+25 2.501819e+25 6.679857e+24 9.238891e+24 6.107859e+24 5.8806e+24 3.962256e+24 3.127274e+24 8.349822e+23 1.154861e+24 7.634824e+23 0.1298307 5.92698e+23 4.973145e-10 0.0003053624 2.123589e+12 8157380 7.716593e+08 3.573723e-07 2.354505e-13 3.223566e-20 0.5 0.5 0.04107317 1 6.6521 7.209709e+26 2.301694e+28 +5500 1273 1e+19 0 5e-06 4.752e+25 3.194756e+25 2.522461e+25 6.722947e+24 9.295291e+24 6.27715e+24 5.94e+24 3.993445e+24 3.153077e+24 8.403683e+23 1.161911e+24 7.846438e+23 0.1320949 5.915857e+23 4.987071e-10 0.0003073569 2.064174e+12 8443412 8.053538e+08 3.624791e-07 2.422277e-13 3.363743e-20 0.5 0.5 0.0416601 1 6.719293 7.209709e+26 2.301694e+28 diff --git a/utilities/postProcessing/sciantix.py b/utilities/postProcessing/sciantix.py deleted file mode 100644 index bf11d663..00000000 --- a/utilities/postProcessing/sciantix.py +++ /dev/null @@ -1,606 +0,0 @@ -""" -sciantix.py is a python module made to handle the sciantix (standalone) postprocessing, -and plot the quantities in the output.txt file -the purposes are: - - to plot variables, choosing both x- and y- axes (is_main = 1) - - to prepare quantities to be plotted (is_main = 2) - -@author: Giovanni Zullo -@author: C Valot - -Instructions: -- run sciantix.py in a folder containing the output.txt file - -""" - -# Importing necessary libraries -import numpy as np -import os -import importlib -import tkinter as tk -from tkinter import messagebox -from matplotlib.backends.backend_tkagg import FigureCanvasTkAgg -import matplotlib.pyplot as plt -from matplotlib.figure import Figure -import matplotlib.gridspec as gridspec -import tkinter as tk -from tkinter import messagebox -from matplotlib.figure import Figure -from matplotlib.backends.backend_tkagg import FigureCanvasTkAgg -import matplotlib.pyplot as plt -import sys - - -# Colors for the plots -colors = ["blue", "red", "green", "orange", "purple", "brown", "pink", "gray", "olive", "cyan"] -canvas = None # Declare canvas as a global variable -canvas_closed = False # Flag to track if sciantix window was closed - -is_main = 0 - -""" Defining useful functions """ -# Function to check if given file is present in the current folder -def is_output_here(filename): - try: - f = open(filename) # Try opening the file - except: - print("ERROR: ", filename, " not found!") # If file not found, print error - return False - else: - f.close() # Close the file if found - return True - -# Function to import a .txt file into a numpy array -def import_data(filename): - """ - This function import a .txt file into an ndarray - """ - - if(is_output_here(filename) is False): - return # If file not found, return None - data = np.genfromtxt(filename, dtype= 'str', delimiter='\t') # Convert the file data to numpy array - return data - -# Function to get the column index of a given variable in the ndarray -def findSciantixVariablePosition(output, variable_name): - """ - This function gets the output.txt file and the variable name, - giving back its column index in the ndarray - """ - - i,j = np.where(output == variable_name) # Find index where variable_name exists in 'output' - return int(j) # Return the column index - -# Function to set the working directory to the folder that contains the sciantix file "output.txt" -def working_dir(path): - """ - This function receives the path of the folder that contains the sciantix file "output.txt". - If output.txt is in the same folder of sciantix.py, it is not necessary to use this function. - """ - os.chdir(path) # Change the current working directory to 'path' - return None - -# Function to print the names of the sciantix quantities in output.txt that can be plotted -def getDictionary(file): - """ - ---------------- - Input parameters - ---------------- - - output_filename : TYPE = str - - name of the output file (e.g. 'output.txt') - the output file must be in the sciantix.py directory or - the path must de defined by sciantix.working_dir(path). - - default name = 'output.txt' - - ------- - Returns - ------- - The names of the sciantix quantities in output.txt that can be plotted - and the corresponding values for the plot positions. - """ - - if(is_output_here(file) is False): - return # If file not found, return None - - data = import_data(file) # Import the file data - output_tags = data[0,:-1] # Extract the output tags (column headers) from the first row - data_shape = data.shape # Get the shape of the data array (rows, columns) - tag_positions = np.linspace(0, data_shape[1] - 2, data_shape[1] - 1) # Generate positions for the tags - - print(f"An " + file + " file has been detected in the current folder.") - print("The file ", file, "contains the following variables:") - print("") - - for i in range(0, data_shape[1] - 1): - print("Position #", tag_positions[i].astype(int), ", variable = ", output_tags[i]) # Print the positions and variable names - return output_tags - -def sciantix(file, is_main): - # Define the sciantix function which accepts two parameters: the file to be processed and a flag indicating - # whether this function is called from the main script (is_main == 1) or not (is_main == 0). - - global canvas # Indicate that we're using the global 'canvas' variable, not creating a local one. - - output_filename = file # Name of the file to process. - output_tags = getDictionary(output_filename) # Get the tags (column headers) from the file. - root = tk.Tk() # Initialize a Tkinter root window. - - # Set initial size and position of the Tkinter window. - root.geometry("800x600+100+50") - - def plot_graph(): - # Nested function to plot the graph based on selected x and y tags from listboxes. - if not listbox_x.curselection() or not listbox_y.curselection(): - # If either of the listboxes does not have a selection, show a warning message and return. - messagebox.showwarning("Selection error", "Please select an item from both lists.") - return - - # Get the indices of the selected x and y tags. - x_index = listbox_x.curselection()[0] - y_indices = list(listbox_y.curselection()) - - # Get the actual tag names based on these indices. - x_name = output_tags[x_index] - y_names = [output_tags[i] for i in y_indices] - - # Adjust figure width based on number of y-axes. - fig_width = 10 + 0.75 * len(y_names) - fig = Figure(figsize=(fig_width, 6)) # Create a matplotlib Figure with the adjusted width. - fig.subplots_adjust(right=0.75 / fig_width * 10) # Adjust right side of figure layout. - ax = fig.add_subplot(111) # Add a subplot to the figure. - - # Loop over each y tag. - for i, y_name in enumerate(y_names): - color = colors[i % len(colors)] # Pick a color for this y-axis plot. - new_ax = ax if i == 0 else ax.twinx() # If this is the first y tag, use the existing ax, otherwise create a new y-axis. - if i >= 1: # Make the spacing for the extra axes - new_pos = 1.0 + 0.2 * i - new_ax.spines['right'].set_position(('axes', new_pos)) # Position the y-axis. - plot(x_name, y_name, output_filename, new_ax, color) # Call the plot function to draw this y-axis plot. - new_ax.set_ylabel(y_name, color=color) # Set the y label and its color. - - # If a matplotlib canvas already exists, forget its grid. - global canvas - if canvas: - canvas.get_tk_widget().grid_forget() - - # Create a new Tkinter canvas widget and place it in the grid. - tk_canvas = tk.Canvas(root) - tk_canvas.grid(row=1, column=0, columnspan=3, sticky="nsew") - - # Add a horizontal scrollbar attached to the new Tkinter canvas and place it in the grid. - scrollbar_x = tk.Scrollbar(root, command=tk_canvas.xview, orient="horizontal") - scrollbar_x.grid(row=2, column=0, columnspan=3, sticky="ew") - - tk_canvas.configure(xscrollcommand=scrollbar_x.set) # Configure the canvas to update the scrollbar. - - # Create a new matplotlib canvas and draw. - canvas = FigureCanvasTkAgg(fig, master=tk_canvas) - canvas.draw() - - # Pack the matplotlib canvas into the Tkinter canvas. - canvas.get_tk_widget().pack(side="top", fill="both", expand=True) - - # Attach the matplotlib canvas to the Tkinter canvas. - tk_canvas.create_window(0, 0, window=canvas.get_tk_widget(), anchor="nw") - - # Update the scroll region after the width and height of the thing inside the canvas changes. - tk_canvas.configure(scrollregion=tk_canvas.bbox("all")) - - # Give more weight to the rows that contain the canvas and the scroll bar. - root.grid_rowconfigure(1, weight=1) - root.grid_rowconfigure(2, weight=0) - root.grid_columnconfigure(0, weight=1) - - # Clear the selection in the y-axis listbox after plotting. - listbox_y.selection_clear(0, 'end') - - # Define two different versions of the function 'hide_window' depending on the value of 'is_main'. - if is_main == 0 : - def hide_window(): - # If this function is not called from the main script, just withdraw (hide) the root window. - root.withdraw() - - if is_main == 1 : - def hide_window(): - # If this function is called from the main script, set the 'canvas_closed' flag to True, - # quit the mainloop, and destroy the root window. - global canvas_closed - canvas_closed = True - root.quit() - root.destroy() - - # Override default window-closing behavior with the 'hide_window' function. - root.protocol('WM_DELETE_WINDOW', hide_window) - - # Create a listbox for the x-axis tags and place it in the grid. - listbox_x = tk.Listbox(root, exportselection=0, width=50) - listbox_x.grid(row=0, column=0, sticky="nsew") - - # Create a button that calls the 'plot_graph' function when clicked and place it in the grid. - button = tk.Button(root, text="Plot graph", command=plot_graph) - button.grid(row=0, column=1) - - # Create a listbox for the y-axis tags and place it in the grid. - listbox_y = tk.Listbox(root, selectmode=tk.MULTIPLE, exportselection=0, width=50) - listbox_y.grid(row=0, column=2, sticky="nsew") - - # Insert all tags into both listboxes. - for tag in output_tags: - listbox_x.insert(tk.END, tag) - listbox_y.insert(tk.END, tag) - - # Start the Tkinter main event loop. - root.mainloop() - -def plot(x_name, y_name, output_filename="output.txt", ax=None, color='blue'): - # Define the plot function, which takes in the x and y tag names, the file name (default is 'output.txt'), - # an optional Axes object on which to plot, and a color for the line. - - # verify if output file exists - if(is_output_here(output_filename) is False): - # If the file does not exist, return without doing anything. - return - - # Read the data from the file. - data = import_data(output_filename) - - # Extract the x and y data from the appropriate columns and convert to float. - x = data[1:,findSciantixVariablePosition(data, x_name)].astype(float) - y = data[1:,findSciantixVariablePosition(data, y_name)].astype(float) - - # Plot the y data against the x data on the provided axes (or on new axes if none were provided). - ax.plot(x, y, color=color, label=y_name) - - # Set the labels for the x and y axes and color the y-axis label. - ax.set_xlabel(x_name) - ax.set_ylabel(y_name, color=color) - ax.tick_params(axis='y', colors=color) # Also color the y-axis tick labels. - - -def plot_data(ax, xAxis, data, axisLabel, legendLabel, color, line_style='-', - axis_id='y1', secondary_axes=None, y_limits=None, x_limits=None): - """ - Plots data on the given axis, handling multiple secondary axes and axis limits. - Includes the ability to specify the line style. - Uses axis_id as a unique identifier for secondary axes. - The first secondary axis ('y2') is attached to the main plot frame, - and subsequent secondary axes are pushed to the right. - """ - if secondary_axes is None: - secondary_axes = {} - - if axis_id == 'y1': - ax.plot(xAxis, data, label=legendLabel, color=color, linestyle=line_style) - ax.set_ylabel(axisLabel, color=color) - ax.tick_params(axis='y', labelcolor=color) # Set tick color for primary y-axis - if y_limits: - ax.set_ylim(y_limits) - if x_limits: - ax.set_xlim(x_limits) - else: - if axis_id not in secondary_axes: - new_ax = ax.twinx() - secondary_axes[axis_id] = new_ax - new_ax.set_ylabel(axisLabel, color=color) - - # Adjust position for additional secondary axes beyond the first one - if axis_id != 'y2': - ax_position = ax.get_position() - new_ax.set_position([ax_position.x0, ax_position.y0, - ax_position.width, ax_position.height]) - offset = 60 * (len(secondary_axes) - 1) # Offset for additional axes - new_ax.spines['right'].set_position(('outward', offset)) - - existing_ax = secondary_axes[axis_id] - existing_ax.plot(xAxis, data, label=legendLabel, color=color, linestyle=line_style) - existing_ax.tick_params(axis='y', labelcolor=color) - if y_limits: - existing_ax.set_ylim(y_limits) - if x_limits: - existing_ax.set_xlim(x_limits) - - return ax, secondary_axes - -def sciantix_dictionary(file): - data = import_data(file) - - variable_labels = { - "t": "Time (h)", - "T": "Temperature (K)", - "frate": "Fission rate (fiss / m3 s)", - "sigma": "Hydrostatic stress (MPa)", - "bu": "Burnup (MWd/kgUO2)", - "N": "Intergranular bubble concentration (bub/m2)", - "n": "Intergranular atoms per bubble (at/bub)", - "v": "Intergranular vacancies per bubble (vac/bub)", - "rad": "Intergranular bubble radius (m)", - "A": "Intergranular bubble area (m2)", - "vol": "Intergranular bubble volume (m3)", - "fc": "Intergranular fractional coverage (/)", - "fcsat": "Intergranular saturation fractional coverage (/)", - "f": "Intergranular fractional intactness (/)", - "fv": "Intergranular vented fraction (/)", - "pv": "Intergranular venting probability (/)", - "xe_p": "Xe produced (at/m3)", - "xe_ig": "Xe in grain (at/m3)", - "xe_igHBS": "Xe in grain HBS (at/m3)", - "xe_igb": "Xe in intragranular bubbles (at/m3)", - "xe_igs": "Xe in intragranular solution (at/m3)", - "xe_gb": "Xe at grain boundary (at/m3)", - "xe_r": "Xe released (at/m3)", - "fgr" : "Fission gas release (/)", - "alpha": "Restructured volume fraction (/)", - "sv": "Intergranular S/V (1/m)", - "swe_gb" : "Intergranular gas swelling (/)", - "a": "Grain radius (m)", - } - - sd = {} - label = [] - name = [] - - for var_name, var_label in variable_labels.items(): - label.append(var_label) - name.append(var_name) - - for i in range(len(label)): - try: - var_index = findSciantixVariablePosition(data, label[i]) - except: - var_index = None - if var_index is not None: - sd[name[i]] = data[1:, var_index].astype(float) - else: - sd[name[i]] = np.zeros_like(data[1:, 0].astype(float)) - print(f"Variable '{label[i]}' not found in the data.") - - return sd - -def plot(sd): - - # Plot : input history - fig, ax = plt.subplots() - ax.set_xlabel('Time, h') - secondary_axes_1 = {} - ax, _ = plot_data(ax, sd["t"], sd["T"], 'Temperature (K)', 'T', 'tab:red', '-', 'y1') - ax, secondary_axes_1 = plot_data(ax, sd["t"], sd["frate"], 'Fission rate (fiss / m3 s)', 'F', 'tab:blue','-', 'y2', secondary_axes_1) - ax, secondary_axes_1 = plot_data(ax, sd["t"], sd["sigma"], 'Hydrostatic stress (MPa)', 's_h', 'tab:green','-', 'y3', secondary_axes_1) - fig.tight_layout() - - plt.show() - - # Plot : Xenon - fig, ax = plt.subplots() - ax.set_xlabel('Time, h') - - ax.plot(sd["t"], sd["xe_p"], color=colors[0], label="Xe produced (at/m3)") - ax.plot(sd["t"], sd["xe_ig"], color=colors[1], label="Xe in grain (at/m3)") - ax.plot(sd["t"], sd["xe_igs"], color=colors[2], label="Xe in intragranular solution (at/m3)") - ax.plot(sd["t"], sd["xe_igb"], color=colors[3], label="Xe in intragranular bubbles (at/m3)") - ax.plot(sd["t"], sd["xe_gb"], color=colors[6], label="Xe at grain boundary (at/m3)") - ax.plot(sd["t"], sd["xe_r"], color=colors[5], label="Xe released (at/m3)") - - # ax.set_yscale('log') - ax.set_ylabel("Xe concentrations") - ax.tick_params(axis='y') - ax.legend() - fig.tight_layout() - plt.show() - - # plot: HBS in grain - fig, ax1 = plt.subplots() - - ax1.plot(sd["t"], sd["xe_ig"], color='blue', label='xe_ig') - ax1.plot(sd["t"], sd["xe_igHBS"], color='green', label='xe_ig_HBS') - ax1.set_xlabel('Time') - ax1.set_ylabel('Xe in grain', color='black') - ax2 = ax1.twinx() - ax2.plot(sd["t"], sd["alpha"], color='orange', label='restructured volume fraction') - ax2.set_ylabel('alpha', color='black') - ax1.legend(loc='upper left') - ax2.legend(loc='upper right') - plt.show() - - # fig.tight_layout() - plt.show() - - # Plot: burnup - gas in grain - fig, ax1 = plt.subplots() - - ax1.plot(sd["bu"], sd["xe_ig"], color='green', label='xe_ig') - ax1.plot(sd["bu"], sd["xe_igHBS"], color='red', label='xe_igHBS') - ax1.set_xlabel('Burnup') - ax1.set_ylabel('Xe in grain (at/m${}^3$)', color='black') - ax2 = ax1.twinx() - ax2.plot(sd["bu"], sd["alpha"], color='orange', label='alpha') - ax2.set_ylabel('alpha', color='black') - plt.show() - - # fig.tight_layout() - plt.show() - - # Plot: N-A - fig, ax = plt.subplots() - ax.set_xlabel('Intergranular bubble area ($\mu m^2$)') - ax.set_ylabel('Intergranular bubble concentration ($\mu m^{-2}$)') - ax.plot(sd["A"]*1e12, sd["N"]*1e-12, color=colors[4]) - ax.tick_params(axis='y') - fig.tight_layout() - ax.set_xscale('log') - ax.set_yscale('log') - ax.set_xlim(1e-3, 10) - ax.set_ylim(1e-2, 100) - plt.show() - - # Plot: Temperature - Bubble area and concentration - fig, ax = plt.subplots() - ax.set_xlabel('Temperature (K)') - secondary_axes_1 = {} - - ax, _ = plot_data(ax, sd["T"], sd["A"], 'Intergranular bubble area', 'A', 'tab:red', '-', 'y1') - ax, secondary_axes_1 = plot_data(ax, sd["T"], sd["N"], 'Intergranular bubble concentration', 'N', 'tab:blue','-', 'y2', secondary_axes_1) - - # fig.tight_layout() - plt.show() - - # Plot: Time - vacancies and atoms - fig, ax = plt.subplots() - ax.set_xlabel('Time (h)') - secondary_axes_1 = {} - - ax, _ = plot_data(ax, sd["t"], sd["v"], 'Intergranular vacancies per bubble', 'N', 'tab:red', '-', 'y1') - ax, secondary_axes_1 = plot_data(ax, sd["t"], sd["n"], 'Intergranular atoms per bubble', 'n_g', 'tab:blue','-', 'y2', secondary_axes_1) - - # fig.tight_layout() - plt.show() - - # Plot: Temperature - vacancies and atoms - fig, ax = plt.subplots() - ax.set_xlabel('Temperature (K)') - secondary_axes_1 = {} - - ax, _ = plot_data(ax, sd["T"], sd["v"], 'Intergranular vacancies per bubble', 'N', 'tab:red', '-', 'y1') - ax, secondary_axes_1 = plot_data(ax, sd["T"], sd["n"], 'Intergranular atoms per bubble', 'n_g', 'tab:blue','-', 'y2', secondary_axes_1) - - # fig.tight_layout() - plt.show() - - # Plot - Time - Intergranular parameters - fig, ax = plt.subplots() - ax.set_xlabel('Time (h)') - - ax.plot(sd["t"], np.ones_like(sd["t"]) * 0.5, color=colors[5], label="Saturation fractional coverage") - ax.plot(sd["t"], sd["fc"], color=colors[0], label="Intergranular fractional coverage") - ax.plot(sd["t"], sd["f"], color=colors[1], label="Intergranular fractional intactness") - ax.plot(sd["t"], sd["fv"], color=colors[2], label="Intergranular vented fraction") - ax.plot(sd["t"], sd["pv"], color=colors[3], label="Intergranular venting probability") - ax.plot(sd["t"], sd["swe_gb"], color=colors[4], label="Intergranular gas swelling") - - ax.tick_params(axis='y') - ax.legend() - - fig.tight_layout() - - plt.show() - - # PLOT - Temperature - Intergranular parameters - fig, ax = plt.subplots() - ax.set_xlabel('Temperature (K)') - - ax.plot(sd["T"], np.ones_like(sd["t"]) * 0.5, color=colors[5], label="Saturation fractional coverage") - ax.plot(sd["T"], sd["fc"], color=colors[0], label="Intergranular fractional coverage") - ax.plot(sd["T"], sd["f"], color=colors[1], label="Intergranular fractional intactness") - ax.plot(sd["T"], sd["fv"], color=colors[2], label="Intergranular vented fraction") - ax.plot(sd["T"], sd["pv"], color=colors[3], label="Intergranular venting probability") - ax.plot(sd["T"], sd["swe_gb"], color=colors[4], label="Intergranular gas swelling") - - ax.tick_params(axis='y') - ax.legend() - - fig.tight_layout() - - plt.show() - - # PLOT: Vented fraction:Fractional coverage - fig, ax = plt.subplots() - ax.set_xlabel('Intergranular fractional coverage') - ax.set_ylabel("Intergranular vented fraction") - - ax.plot(sd["fc"], sd["fv"], color=colors[0], label="Intergranular fractional coverage (/)") - - ax.tick_params(axis='y') - ax.legend() - - fig.tight_layout() - - plt.show() - - # PLOT: Time:FGR - fig, ax = plt.subplots() - ax.plot(sd["t"], sd["fgr"], color=colors[0], label="FGR") - ax.tick_params(axis='y') - ax.legend() - fig.tight_layout() - plt.show() - - # PLOT: Time:burnup - fig, ax = plt.subplots() - - ax.plot(sd["t"], sd["bu"]/0.8814,color=colors[0], label="Burnup") - - ax.tick_params(axis='y') - ax.legend() - - fig.tight_layout() - - plt.show() - - # PLOT: S/V and grain radius - temperature - fig, ax = plt.subplots() - ax.set_xlabel('Temperature (K)') - secondary_axes_1 = {} - ax, _ = plot_data(ax, sd["t"], sd["sv"], 'S/V (1/m)', 'SV', 'tab:red', '-', 'y1') - ax, secondary_axes_1 = plot_data(ax, sd["t"], sd["a"], 'Grain radius (m)', 'a', 'tab:blue','-', 'y2', secondary_axes_1) - fig.tight_layout() - plt.show() - - # PLOT: S/V and grain radius - time - fig, ax = plt.subplots() - ax.set_xlabel('Time, h') - secondary_axes_1 = {} - - ax, _ = plot_data(ax, sd["t"], sd["sv"], 'S/V (1/m)', 'SV', 'tab:red', '-', 'y1') - ax, secondary_axes_1 = plot_data(ax, sd["t"], sd["a"], 'Grain radius (m)', 'a', 'tab:blue','-', 'y2', secondary_axes_1) - fig.tight_layout() - - plt.show() - - # PLOT MMS - # fig, ax = plt.subplots() - # ax.set_xlabel('Time, h') - - # ax.plot(x, xe_gb * 1e2, 'd', color=colors[2], label="MMS: B(t) = P/100") - # ax.plot(x, x3 * 1e17, 'o', color=colors[1], label="MMS: v(t) = P*1e-17") - # ax.plot(x, x2 * ngb * SV * 1e2, '+', color=colors[4], label="MMS: n(t) = B(t) / (N S/V)") - - # ax.plot(x, xe_p, color=colors[0], label="P(t)") - - # ax2 = ax.twinx() - # ax2.set_ylabel('-') - # ax2.plot(x, vol / (4.09e-29 * 1e-17 + 8.48e-29 * 1/100 / (ngb * SV)), color='red', label='V(t) = wn(t) + Wv(t)') - # ax2.plot(x, (4/3 * 3.14 * rad**3 * 0.168610764) / (4.09e-29 * 1e-17 + 8.48e-29 * 1/100 / (ngb * SV)) , color='green', label='r(t)=(3/(4 pi f)V)^(1/3)') - - # ax.tick_params(axis='y') - # ax2.tick_params(axis='y') - # ax.legend(loc='upper left') - # ax2.legend(loc='upper right') - - # fig.tight_layout() - - # plt.show() - -def main(): - is_main = int(input("plot mode (1 or 2): ")) - - os.system('./sciantix.x > log.sciantix') - - if 'output.txt' in os.listdir(os.getcwd()): - - if is_main == 1: - sciantix('output.txt', is_main) - if canvas_closed: - sys.exit() - - elif is_main == 2: - dict = sciantix_dictionary('output.txt') - plot(dict) - else: - print('No file named "output.txt" found in the current directory') - -if __name__ == "__main__": - main() - diff --git a/utilities/postProcessing/sciantix_gui.py b/utilities/postProcessing/sciantix_gui.py new file mode 100644 index 00000000..cb4d78df --- /dev/null +++ b/utilities/postProcessing/sciantix_gui.py @@ -0,0 +1,192 @@ +""" +sciantix_gui.py is a python module made to handle the sciantix (standalone) postprocessing, +and plot the quantities in the output.txt file +the purpose is to plot variables, choosing both x- and y- axes + +@author: G. Zullo +@author: C. Valot + +Instructions: +- run sciantix.py in a folder containing the output.txt file + +""" + +# Importing necessary libraries +import numpy as np +import os +import logging +import tkinter as tk +from tkinter import messagebox +from matplotlib.backends.backend_tkagg import FigureCanvasTkAgg +from matplotlib.figure import Figure +import matplotlib.pyplot as plt +import sys + +# Initialize logging +logging.basicConfig(level=logging.INFO, format='%(levelname)s: %(message)s') + +# Colors for the plots +COLORS = ["blue", "red", "green", "orange", "purple", "brown", "pink", "gray", "olive", "cyan"] + +""" Utility Functions """ + +def is_output_here(filename): + """ + Check if a given file is present in the current folder. + """ + if os.path.isfile(filename): + return True + logging.error(f"{filename} not found!") + return False + +def import_data(filename): + """ + Import a .txt file into an ndarray. + """ + if not is_output_here(filename): + return None + return np.genfromtxt(filename, dtype='str', delimiter='\t') + +def find_sciantix_variable_position(output, variable_name): + """ + Get the column index of a given variable in the ndarray. + """ + try: + _, j = np.where(output == variable_name) + return int(j) + except ValueError: + logging.error(f"Variable '{variable_name}' not found in the data.") + return None + +def get_dictionary(file): + """ + Print the names of the sciantix quantities in output.txt that can be plotted. + """ + data = import_data(file) + if data is None: + return None + + output_tags = data[0, :-1] + tag_positions = np.arange(len(output_tags)) + + logging.info(f"Detected {file} in the current folder with the following variables:") + for i, tag in enumerate(output_tags): + print(f"Position #{tag_positions[i]}, variable = {tag}") + return output_tags + +def create_axes(fig, ax, index, label, color): + """ + Helper function to create a new axis or adjust an existing one. + """ + new_ax = ax if index == 0 else ax.twinx() + if index >= 1: + new_pos = 1.0 + 0.2 * index + new_ax.spines['right'].set_position(('axes', new_pos)) + new_ax.set_ylabel(label, color=color) + return new_ax + +def plot(x_name, y_name, output_filename="output.txt", ax=None, color='blue'): + """ + Plot data from specified x and y columns of the output file. + """ + if not is_output_here(output_filename): + return + + data = import_data(output_filename) + if data is None: + return + + x_index = find_sciantix_variable_position(data, x_name) + y_index = find_sciantix_variable_position(data, y_name) + + if x_index is None or y_index is None: + logging.error("Unable to plot due to missing variable.") + return + + x = data[1:, x_index].astype(float) + y = data[1:, y_index].astype(float) + ax.plot(x, y, color=color, label=y_name) + ax.set_xlabel(x_name) + ax.set_ylabel(y_name, color=color) + ax.tick_params(axis='y', colors=color) + +class SciantixPlotter: + def __init__(self, output_filename): + self.output_filename = output_filename + self.canvas = None + self.root = tk.Tk() + self.output_tags = get_dictionary(output_filename) + + # Corrected condition to check if output_tags is not None and has elements + if self.output_tags is not None and self.output_tags.size > 0: + self.setup_gui() + + def setup_gui(self): + """ + Sets up the Tkinter GUI. + """ + self.root.geometry("800x600+100+50") + self.root.protocol('WM_DELETE_WINDOW', self.hide_window) + + # Create listboxes for selecting x and y variables + self.listbox_x = tk.Listbox(self.root, exportselection=0, width=50) + self.listbox_x.grid(row=0, column=0, sticky="nsew") + + self.button = tk.Button(self.root, text="Plot graph", command=self.plot_graph) + self.button.grid(row=0, column=1) + + self.listbox_y = tk.Listbox(self.root, selectmode=tk.MULTIPLE, exportselection=0, width=50) + self.listbox_y.grid(row=0, column=2, sticky="nsew") + + for tag in self.output_tags: + self.listbox_x.insert(tk.END, tag) + self.listbox_y.insert(tk.END, tag) + + def hide_window(self): + """ + Handles the window close event. + """ + self.root.quit() + self.root.destroy() + + def plot_graph(self): + """ + Handle plotting logic with dynamic figure and axes. + """ + x_index = self.listbox_x.curselection() + y_indices = self.listbox_y.curselection() + + if not x_index or not y_indices: + messagebox.showwarning("Selection error", "Please select an item from both lists.") + return + + x_name = self.output_tags[x_index[0]] + y_names = [self.output_tags[i] for i in y_indices] + + fig = Figure(figsize=(10 + 0.75 * len(y_names), 6)) + ax = fig.add_subplot(111) + + for i, y_name in enumerate(y_names): + color = COLORS[i % len(COLORS)] + new_ax = create_axes(fig, ax, i, y_name, color) + plot(x_name, y_name, self.output_filename, new_ax, color) + + if self.canvas: + self.canvas.get_tk_widget().grid_forget() + + self.canvas = FigureCanvasTkAgg(fig, master=self.root) + self.canvas.draw() + self.canvas.get_tk_widget().grid(row=1, column=0, columnspan=3, sticky="nsew") + + def mainloop(self): + """ + Starts the Tkinter main loop. + """ + self.root.mainloop() + +def main(): + plotter = SciantixPlotter('output.txt') + plotter.mainloop() + +if __name__ == "__main__": + main() diff --git a/utilities/postProcessing/sciantix_plot.py b/utilities/postProcessing/sciantix_plot.py new file mode 100644 index 00000000..06c466a5 --- /dev/null +++ b/utilities/postProcessing/sciantix_plot.py @@ -0,0 +1,215 @@ +""" +sciantix_plot.py is a Python script to plot default Sciantix (standalone) quantities + +Instructions: +- Run sciantix_plot.py in a folder containing the output.txt file. + +@author: Giovanni Zullo +""" + +# Importing necessary libraries +import numpy as np +import os +import logging +import tkinter as tk +from tkinter import messagebox +import matplotlib.pyplot as plt +from matplotlib.backends.backend_tkagg import FigureCanvasTkAgg +from matplotlib.figure import Figure + +# Configure logging +logging.basicConfig(level=logging.INFO, format='%(asctime)s - %(levelname)s - %(message)s') + +# Color palette for plots +colors = ["blue", "red", "green", "orange", "purple", "brown", "pink", "gray", "olive", "cyan"] + +def is_output_here(filename): + """ + Check if a given file is present in the current folder. + """ + if os.path.isfile(filename): + return True + logging.error(f"{filename} not found!") + return False + +def import_data(filename): + """ + This function imports a .txt file into an ndarray. + """ + if not is_output_here(filename): + logging.error(f"File {filename} not found in the directory.") + return None # Return None if file not found + + try: + data = np.genfromtxt(filename, dtype='str', delimiter='\t') # Convert the file data to numpy array + return data + except Exception as e: + logging.error(f"Error reading {filename}: {str(e)}") + return None + +def find_sciantix_variable_position(output, variable_name): + """ + This function gets the output.txt file and the variable name, + giving back its column index in the ndarray. + """ + try: + i, j = np.where(output == variable_name) # Find index where variable_name exists in 'output' + return int(j) # Return the column index + except: + logging.error(f"Variable {variable_name} not found in the output data.") + return None + +def working_dir(path): + """ + This function receives the path of the folder that contains the sciantix file "output.txt". + If output.txt is in the same folder of sciantix.py, it is not necessary to use this function. + """ + os.chdir(path) # Change the current working directory to 'path' + logging.info(f"Working directory set to: {path}") + return None + +def plot_data(ax, xAxis, data, axisLabel, legendLabel, color, line_style='-', + axis_id='y1', secondary_axes=None, y_limits=None, x_limits=None): + """ + Plots data on the given axis, handling multiple secondary axes and axis limits. + Includes the ability to specify the line style. + Uses axis_id as a unique identifier for secondary axes. + The first secondary axis ('y2') is attached to the main plot frame, + and subsequent secondary axes are pushed to the right. + """ + if secondary_axes is None: + secondary_axes = {} + + if axis_id == 'y1': + ax.plot(xAxis, data, label=legendLabel, color=color, linestyle=line_style) + ax.set_ylabel(axisLabel, color=color) + ax.tick_params(axis='y', labelcolor=color) # Set tick color for primary y-axis + if y_limits: + ax.set_ylim(y_limits) + if x_limits: + ax.set_xlim(x_limits) + else: + if axis_id not in secondary_axes: + new_ax = ax.twinx() + secondary_axes[axis_id] = new_ax + new_ax.set_ylabel(axisLabel, color=color) + + # Adjust position for additional secondary axes beyond the first one + if axis_id != 'y2': + ax_position = ax.get_position() + new_ax.set_position([ax_position.x0, ax_position.y0, + ax_position.width, ax_position.height]) + offset = 60 * (len(secondary_axes) - 1) # Offset for additional axes + new_ax.spines['right'].set_position(('outward', offset)) + + existing_ax = secondary_axes[axis_id] + existing_ax.plot(xAxis, data, label=legendLabel, color=color, linestyle=line_style) + existing_ax.tick_params(axis='y', labelcolor=color) + if y_limits: + existing_ax.set_ylim(y_limits) + if x_limits: + existing_ax.set_xlim(x_limits) + + return ax, secondary_axes + +def sciantix_dictionary(file): + data = import_data(file) + if data is None: + return {} + + variable_labels = { + "t": "Time (h)", + "T": "Temperature (K)", + "frate": "Fission rate (fiss / m3 s)", + "sigma": "Hydrostatic stress (MPa)", + "bu": "Burnup (MWd/kgUO2)", + "N": "Intergranular bubble concentration (bub/m2)", + "n": "Intergranular atoms per bubble (at/bub)", + "v": "Intergranular vacancies per bubble (vac/bub)", + "rad": "Intergranular bubble radius (m)", + "A": "Intergranular bubble area (m2)", + "vol": "Intergranular bubble volume (m3)", + "fc": "Intergranular fractional coverage (/)", + "fcsat": "Intergranular saturation fractional coverage (/)", + "f": "Intergranular fractional intactness (/)", + "fv": "Intergranular vented fraction (/)", + "pv": "Intergranular venting probability (/)", + "xe_p": "Xe produced (at/m3)", + "xe_ig": "Xe in grain (at/m3)", + "xe_igHBS": "Xe in grain HBS (at/m3)", + "xe_igb": "Xe in intragranular bubbles (at/m3)", + "xe_igs": "Xe in intragranular solution (at/m3)", + "xe_gb": "Xe at grain boundary (at/m3)", + "xe_r": "Xe released (at/m3)", + "fgr" : "Fission gas release (/)", + "alpha": "Restructured volume fraction (/)", + "sv": "Intergranular S/V (1/m)", + "swe_gb" : "Intergranular gas swelling (/)", + "a": "Grain radius (m)", + } + + sd = {} + label = [] + name = [] + + for var_name, var_label in variable_labels.items(): + label.append(var_label) + name.append(var_name) + + for i in range(len(label)): + try: + var_index = find_sciantix_variable_position(data, label[i]) + except: + var_index = None + if var_index is not None: + sd[name[i]] = data[1:, var_index].astype(float) + else: + sd[name[i]] = np.zeros_like(data[1:, 0].astype(float)) + logging.warning(f"Variable '{label[i]}' not found in the data.") + + return sd + +def create_plot(x_data, y_data, xlabel, ylabel, legends, colors, title=None, secondary_y=False): + """ + Utility function to create plots. + """ + fig, ax1 = plt.subplots() + ax1.set_xlabel(xlabel) + ax1.set_ylabel(ylabel, color=colors[0]) + + # Primary plot + ax1.plot(x_data, y_data[0], color=colors[0], label=legends[0]) + ax1.tick_params(axis='y', labelcolor=colors[0]) + + if secondary_y: + ax2 = ax1.twinx() + ax2.set_ylabel(legends[1], color=colors[1]) + ax2.plot(x_data, y_data[1], color=colors[1], label=legends[1]) + ax2.tick_params(axis='y', labelcolor=colors[1]) + + # Add legend and title + ax1.legend(loc='upper left') + if secondary_y: + ax2.legend(loc='upper right') + if title: + plt.title(title) + fig.tight_layout() + plt.show() + +def plot(sd): + create_plot( + x_data=sd["t"], + y_data=[sd["xe_p"]], + xlabel='Time, h', + ylabel='Xe produced, at / m3', + legends=['Xe produced, at / m3'], + colors=['tab:red'], + secondary_y=False + ) + +def main(): + data_dict = sciantix_dictionary('output.txt') + plot(data_dict) + +if __name__ == "__main__": + main() From a0ee94776e7a7528ae439500a6b60118608284c7 Mon Sep 17 00:00:00 2001 From: giozu Date: Wed, 28 Aug 2024 11:03:31 +0200 Subject: [PATCH 11/15] input_settings update --- regression/input_settings.txt | 44 ++++++++-------- utilities/InputExplanation.md | 50 +++++++++---------- utilities/inputExample/input_settings.txt | 22 ++++++++ .../inputExample/print_input_settings.py | 44 ++++++++-------- 4 files changed, 91 insertions(+), 69 deletions(-) create mode 100644 utilities/inputExample/input_settings.txt diff --git a/regression/input_settings.txt b/regression/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/input_settings.txt +++ b/regression/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/utilities/InputExplanation.md b/utilities/InputExplanation.md index 7a75743c..cf844e27 100644 --- a/utilities/InputExplanation.md +++ b/utilities/InputExplanation.md @@ -11,38 +11,38 @@ Below is a detailed description of each file. --- -## Input Settings +## Input settings The following settings define the models and methods used for the simulation. ```plaintext -1 # iGrainGrowth (0 = no grain growth, 1 = Ainscough et al. (1973), 2 = Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0 = constant value, 1 = Turnbull et al. (1988)) -1 # iDiffusionSolver (1 = SDA with quasi-stationary hypothesis, 2 = SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1 = Pizzocri et al. (2018)) -1 # iResolutionRate (0 = constant value, 1 = Turnbull (1971), 2 = Losonen (2000), 3 = thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0 = constant value, 1 = Ham (1958)) -1 # iNucleationRate (0 = constant value, 1 = Olander, Wongsawaeng (2006)) -1 # iOutput (1 = default output files) -1 # iGrainBoundaryVacancyDiffusivity (0 = constant value, 1 = Reynolds and Burton (1979), 2 = Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0 = no grain boundary bubbles, 1 = Pastore et al. (2013)) -1 # iGrainBoundaryMicroCracking (0 = no model considered, 1 = Barani et al. (2017)) -0 # iFuelMatrix (0 = UO2, 1 = UO2 + HBS) -0 # iGrainBoundaryVenting (0 = no model considered, 1 = Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0 = not considered) -0 # iHelium (0 = not considered) -0 # iHeDiffusivity (0 = null value, 1 = limited lattice damage, Luzzi et al. (2018), 2 = significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0 = no model considered, 1 = TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0 = no model considered, 1 = fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0 = no evolution of HBS porosity, 1 = HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0 = zero production rate, 1 = helium from ternary fissions, 2 = linear with burnup (FR)) -0 # iStoichiometryDeviation (0 = not considered, 1 = Cox et al. (1986), 2 = Bittel et al. (1969), 3 = Abrefah et al. (1994), 4 = Imamura et al. (1997), 5 = Langmuir-based approach) -0 # iBubbleDiffusivity (0 = not considered, 1 = volume diffusivity) +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) ``` --- -## Input Initial Conditions +## Input initial conditions This file sets the initial conditions for various parameters within the simulation. @@ -79,7 +79,7 @@ This file sets the initial conditions for various parameters within the simulati --- -## Input Scaling Factors +## Input scaling factors This file contains the scaling factors applied to various model parameters during the simulation. diff --git a/utilities/inputExample/input_settings.txt b/utilities/inputExample/input_settings.txt new file mode 100644 index 00000000..cd5811f1 --- /dev/null +++ b/utilities/inputExample/input_settings.txt @@ -0,0 +1,22 @@ +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/utilities/inputExample/print_input_settings.py b/utilities/inputExample/print_input_settings.py index d3a1b3e9..82b7eca6 100644 --- a/utilities/inputExample/print_input_settings.py +++ b/utilities/inputExample/print_input_settings.py @@ -5,25 +5,25 @@ """ with open('input_settings.txt', 'w') as file: - file.write('1\t#\tiGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013))\n') - file.write('1\t#\tiFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988))\n') - file.write('1\t#\tiDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis)\n') - file.write('1\t#\tiIntraGranularBubbleBehavior (1= Pizzocri et al. (2018))\n') - file.write('1\t#\tiResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021))\n') - file.write('1\t#\tiTrappingRate (0= constant value, 1= Ham (1958))\n') - file.write('1\t#\tiNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006))\n') - file.write('1\t#\tiOutput (1= default output files)\n') - file.write('1\t#\tiGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004) \n') - file.write('1\t#\tiGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013))\n') - file.write('1\t#\tiGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017))\n') - file.write('0\t#\tiFuelMatrix (0= UO2, 1= UO2 + HBS)\n') - file.write('0\t#\tiGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE)\n') - file.write('0\t#\tiRadioactiveFissionGas (0= not considered)\n') - file.write('0\t#\tiHelium (0= not considered)\n') - file.write('0\t#\tiHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018))\n') - file.write('0\t#\tiGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model)\n') - file.write('0\t#\tiHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020))\n') - file.write('0\t#\tiHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data)\n') - file.write('0\t#\tiHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR))\n') - file.write('0\t#\tiStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach)\n') - file.write('0\t#\tiBubbleDiffusivity (0= not considered, 1= volume diffusivity)') + file.write('1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013))\n') + file.write('1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988))\n') + file.write('1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis)\n') + file.write('1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018))\n') + file.write('1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021))\n') + file.write('1 # iTrappingRate (0= constant value, 1= Ham (1958))\n') + file.write('1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006))\n') + file.write('1 # iOutput (1= default output files)\n') + file.write('1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004))\n') + file.write('1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013))\n') + file.write('1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017))\n') + file.write('0 # iFuelMatrix (0= UO2, 1= UO2 + HBS)\n') + file.write('0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE)\n') + file.write('0 # iRadioactiveFissionGas (0= not considered)\n') + file.write('0 # iHelium (0= not considered)\n') + file.write('0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018))\n') + file.write('0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model)\n') + file.write('0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020))\n') + file.write('0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data)\n') + file.write('0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR))\n') + file.write('0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach)\n') + file.write('0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity)') From 6ed8fdc659d520a7c242f234623e09c1f2a97195 Mon Sep 17 00:00:00 2001 From: giozu Date: Mon, 2 Sep 2024 11:57:14 +0200 Subject: [PATCH 12/15] minor changes in regression files --- regression/regression_hbs.py | 2 ++ regression/regression_oxidation.py | 4 ++-- 2 files changed, 4 insertions(+), 2 deletions(-) diff --git a/regression/regression_hbs.py b/regression/regression_hbs.py index 5e272aa4..7fb875fd 100644 --- a/regression/regression_hbs.py +++ b/regression/regression_hbs.py @@ -151,6 +151,8 @@ def lassmann_fit(x, threshold=60): ax1.plot(bu_gwd_tu, lassmann_fit(bu_gwd_tu), color='darkorchid', linestyle='--', label='Lassmann fit (bu$_0$ = 60 GWd/tU)') ax1.scatter(data_bu, data_xe, color='navy', edgecolors='black', marker='.', label='Walker data (1999)') ax1.plot(sd["bu"] / 0.8814, sd["xe_ig"] / eq, color='limegreen', linestyle='-.', label='Xe in grains - non HBS') + ax1.plot(sd["bu"] / 0.8814, sd["xe_igs"] / eq, linestyle='-.', label='Xe in dynamic solution') + ax1.plot(sd["bu"] / 0.8814, sd["xe_igb"] / eq, linestyle='-.', label='Xe in intra-granular bubbles') ax1.plot(sd["bu"] / 0.8814, sd["xe_igHBS"] / eq, color='orangered', linestyle=':', label='Xe in grains - HBS') ax1.plot(sd["bu"] / 0.8814, (sd["xe_igHBS"] + sd["xe_ig"]) / eq, color='dimgray', linestyle='-', label='Xe in grains - sum') ax1.legend(loc='upper right', fontsize='medium') diff --git a/regression/regression_oxidation.py b/regression/regression_oxidation.py index 7792246a..4667d763 100644 --- a/regression/regression_oxidation.py +++ b/regression/regression_oxidation.py @@ -86,14 +86,14 @@ def do_plot(time, temperature, stiochiometryDeviation, stiochiometryDeviationDat axT.set_ylabel('Temperature (K)') axT.plot(time, temperature, label="Temperature", color='orange') - ax.set_title(file + ' - Stoichiometry deviation') + # ax.set_title(file + ' - Stoichiometry deviation') ax.set_xlabel('Time (h)') ax.set_ylabel('Stoichiometry deviation (/)') h1, l1 = ax.get_legend_handles_labels() h2, l2 = axT.get_legend_handles_labels() ax.legend(h1+h2, l1+l2) - plt.savefig(file + ' - Stoichiometry deviation.png') + # plt.savefig(file + ' - Stoichiometry deviation.png') plt.show() From b06a7657e318a1b2515c15e8194ab22104248595 Mon Sep 17 00:00:00 2001 From: giozu Date: Mon, 9 Sep 2024 09:56:09 +0200 Subject: [PATCH 13/15] changes --- .../test_Baker1977__1273K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__1373K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__1473K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__1573K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__1673K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__1773K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__1873K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__1973K/input_settings.txt | 44 +++++++++---------- .../test_Baker1977__2073K/input_settings.txt | 44 +++++++++---------- .../test_Kashibe1993_23/input_settings.txt | 44 +++++++++---------- .../test_Kashibe1993_44/input_settings.txt | 44 +++++++++---------- .../test_White2004_4000-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4000-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4000-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4000-4/input_settings.txt | 44 +++++++++---------- .../test_White2004_4000-5/input_settings.txt | 44 +++++++++---------- .../test_White2004_4004-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4004-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4004-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4004-4/input_settings.txt | 44 +++++++++---------- .../test_White2004_4004-5/input_settings.txt | 44 +++++++++---------- .../test_White2004_4004-6/input_settings.txt | 44 +++++++++---------- .../test_White2004_4005-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4005-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4005-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4005-4/input_settings.txt | 44 +++++++++---------- .../test_White2004_4005-5/input_settings.txt | 44 +++++++++---------- .../test_White2004_4064-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4064-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4064-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4064-4/input_settings.txt | 44 +++++++++---------- .../test_White2004_4064-5/input_settings.txt | 44 +++++++++---------- .../test_White2004_4065-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4065-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4065-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4065-4/input_settings.txt | 44 +++++++++---------- .../test_White2004_4065-5/input_settings.txt | 44 +++++++++---------- .../test_White2004_4135-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4135-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4135-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4136-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4136-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4136-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4136-4/input_settings.txt | 44 +++++++++---------- .../test_White2004_4140-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4140-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4162-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4162-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4162-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4162-4/input_settings.txt | 44 +++++++++---------- .../test_White2004_4163-1/input_settings.txt | 44 +++++++++---------- .../test_White2004_4163-2/input_settings.txt | 44 +++++++++---------- .../test_White2004_4163-3/input_settings.txt | 44 +++++++++---------- .../test_White2004_4163-4/input_settings.txt | 44 +++++++++---------- 54 files changed, 1188 insertions(+), 1188 deletions(-) diff --git a/regression/test_Baker1977__1273K/input_settings.txt b/regression/test_Baker1977__1273K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1273K/input_settings.txt +++ b/regression/test_Baker1977__1273K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__1373K/input_settings.txt b/regression/test_Baker1977__1373K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1373K/input_settings.txt +++ b/regression/test_Baker1977__1373K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__1473K/input_settings.txt b/regression/test_Baker1977__1473K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1473K/input_settings.txt +++ b/regression/test_Baker1977__1473K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__1573K/input_settings.txt b/regression/test_Baker1977__1573K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1573K/input_settings.txt +++ b/regression/test_Baker1977__1573K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__1673K/input_settings.txt b/regression/test_Baker1977__1673K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1673K/input_settings.txt +++ b/regression/test_Baker1977__1673K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__1773K/input_settings.txt b/regression/test_Baker1977__1773K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1773K/input_settings.txt +++ b/regression/test_Baker1977__1773K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__1873K/input_settings.txt b/regression/test_Baker1977__1873K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1873K/input_settings.txt +++ b/regression/test_Baker1977__1873K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__1973K/input_settings.txt b/regression/test_Baker1977__1973K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__1973K/input_settings.txt +++ b/regression/test_Baker1977__1973K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Baker1977__2073K/input_settings.txt b/regression/test_Baker1977__2073K/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Baker1977__2073K/input_settings.txt +++ b/regression/test_Baker1977__2073K/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Kashibe1993_23/input_settings.txt b/regression/test_Kashibe1993_23/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Kashibe1993_23/input_settings.txt +++ b/regression/test_Kashibe1993_23/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_Kashibe1993_44/input_settings.txt b/regression/test_Kashibe1993_44/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_Kashibe1993_44/input_settings.txt +++ b/regression/test_Kashibe1993_44/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4000-1/input_settings.txt b/regression/test_White2004_4000-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4000-1/input_settings.txt +++ b/regression/test_White2004_4000-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4000-2/input_settings.txt b/regression/test_White2004_4000-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4000-2/input_settings.txt +++ b/regression/test_White2004_4000-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4000-3/input_settings.txt b/regression/test_White2004_4000-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4000-3/input_settings.txt +++ b/regression/test_White2004_4000-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4000-4/input_settings.txt b/regression/test_White2004_4000-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4000-4/input_settings.txt +++ b/regression/test_White2004_4000-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4000-5/input_settings.txt b/regression/test_White2004_4000-5/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4000-5/input_settings.txt +++ b/regression/test_White2004_4000-5/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4004-1/input_settings.txt b/regression/test_White2004_4004-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4004-1/input_settings.txt +++ b/regression/test_White2004_4004-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4004-2/input_settings.txt b/regression/test_White2004_4004-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4004-2/input_settings.txt +++ b/regression/test_White2004_4004-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4004-3/input_settings.txt b/regression/test_White2004_4004-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4004-3/input_settings.txt +++ b/regression/test_White2004_4004-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4004-4/input_settings.txt b/regression/test_White2004_4004-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4004-4/input_settings.txt +++ b/regression/test_White2004_4004-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4004-5/input_settings.txt b/regression/test_White2004_4004-5/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4004-5/input_settings.txt +++ b/regression/test_White2004_4004-5/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4004-6/input_settings.txt b/regression/test_White2004_4004-6/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4004-6/input_settings.txt +++ b/regression/test_White2004_4004-6/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4005-1/input_settings.txt b/regression/test_White2004_4005-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4005-1/input_settings.txt +++ b/regression/test_White2004_4005-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4005-2/input_settings.txt b/regression/test_White2004_4005-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4005-2/input_settings.txt +++ b/regression/test_White2004_4005-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4005-3/input_settings.txt b/regression/test_White2004_4005-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4005-3/input_settings.txt +++ b/regression/test_White2004_4005-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4005-4/input_settings.txt b/regression/test_White2004_4005-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4005-4/input_settings.txt +++ b/regression/test_White2004_4005-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4005-5/input_settings.txt b/regression/test_White2004_4005-5/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4005-5/input_settings.txt +++ b/regression/test_White2004_4005-5/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4064-1/input_settings.txt b/regression/test_White2004_4064-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4064-1/input_settings.txt +++ b/regression/test_White2004_4064-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4064-2/input_settings.txt b/regression/test_White2004_4064-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4064-2/input_settings.txt +++ b/regression/test_White2004_4064-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4064-3/input_settings.txt b/regression/test_White2004_4064-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4064-3/input_settings.txt +++ b/regression/test_White2004_4064-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4064-4/input_settings.txt b/regression/test_White2004_4064-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4064-4/input_settings.txt +++ b/regression/test_White2004_4064-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4064-5/input_settings.txt b/regression/test_White2004_4064-5/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4064-5/input_settings.txt +++ b/regression/test_White2004_4064-5/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4065-1/input_settings.txt b/regression/test_White2004_4065-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4065-1/input_settings.txt +++ b/regression/test_White2004_4065-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4065-2/input_settings.txt b/regression/test_White2004_4065-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4065-2/input_settings.txt +++ b/regression/test_White2004_4065-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4065-3/input_settings.txt b/regression/test_White2004_4065-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4065-3/input_settings.txt +++ b/regression/test_White2004_4065-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4065-4/input_settings.txt b/regression/test_White2004_4065-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4065-4/input_settings.txt +++ b/regression/test_White2004_4065-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4065-5/input_settings.txt b/regression/test_White2004_4065-5/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4065-5/input_settings.txt +++ b/regression/test_White2004_4065-5/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4135-1/input_settings.txt b/regression/test_White2004_4135-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4135-1/input_settings.txt +++ b/regression/test_White2004_4135-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4135-2/input_settings.txt b/regression/test_White2004_4135-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4135-2/input_settings.txt +++ b/regression/test_White2004_4135-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4135-3/input_settings.txt b/regression/test_White2004_4135-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4135-3/input_settings.txt +++ b/regression/test_White2004_4135-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4136-1/input_settings.txt b/regression/test_White2004_4136-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4136-1/input_settings.txt +++ b/regression/test_White2004_4136-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4136-2/input_settings.txt b/regression/test_White2004_4136-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4136-2/input_settings.txt +++ b/regression/test_White2004_4136-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4136-3/input_settings.txt b/regression/test_White2004_4136-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4136-3/input_settings.txt +++ b/regression/test_White2004_4136-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4136-4/input_settings.txt b/regression/test_White2004_4136-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4136-4/input_settings.txt +++ b/regression/test_White2004_4136-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4140-1/input_settings.txt b/regression/test_White2004_4140-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4140-1/input_settings.txt +++ b/regression/test_White2004_4140-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4140-2/input_settings.txt b/regression/test_White2004_4140-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4140-2/input_settings.txt +++ b/regression/test_White2004_4140-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4162-1/input_settings.txt b/regression/test_White2004_4162-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4162-1/input_settings.txt +++ b/regression/test_White2004_4162-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4162-2/input_settings.txt b/regression/test_White2004_4162-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4162-2/input_settings.txt +++ b/regression/test_White2004_4162-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4162-3/input_settings.txt b/regression/test_White2004_4162-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4162-3/input_settings.txt +++ b/regression/test_White2004_4162-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4162-4/input_settings.txt b/regression/test_White2004_4162-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4162-4/input_settings.txt +++ b/regression/test_White2004_4162-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4163-1/input_settings.txt b/regression/test_White2004_4163-1/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4163-1/input_settings.txt +++ b/regression/test_White2004_4163-1/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4163-2/input_settings.txt b/regression/test_White2004_4163-2/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4163-2/input_settings.txt +++ b/regression/test_White2004_4163-2/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4163-3/input_settings.txt b/regression/test_White2004_4163-3/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4163-3/input_settings.txt +++ b/regression/test_White2004_4163-3/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file diff --git a/regression/test_White2004_4163-4/input_settings.txt b/regression/test_White2004_4163-4/input_settings.txt index 090b1538..cd5811f1 100644 --- a/regression/test_White2004_4163-4/input_settings.txt +++ b/regression/test_White2004_4163-4/input_settings.txt @@ -1,22 +1,22 @@ -1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) -1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) -1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) -1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) -1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) -1 # iTrappingRate (0= constant value, 1= Ham (1958)) -1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) -1 # iOutput (1= default output files) -1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= Pastore et al. (2015)) -1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) -1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) -0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) -0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) -0 # iRadioactiveFissionGas (0= not considered) -0 # iHelium (0= not considered) -0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) -0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) -0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) -0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) -0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) -0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) -0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file +1 # iGrainGrowth (0= no grain growth, 1= Ainscough et al. (1973), 2= Van Uffelen et al. (2013)) +1 # iFissionGasDiffusivity (0= constant value, 1= Turnbull et al. (1988)) +1 # iDiffusionSolver (1= SDA with quasi-stationary hypothesis, 2= SDA without quasi-stationary hypothesis) +1 # iIntraGranularBubbleBehavior (1= Pizzocri et al. (2018)) +1 # iResolutionRate (0= constant value, 1= Turnbull (1971), 2= Losonen (2000), 3= thermal resolution, Cognini et al. (2021)) +1 # iTrappingRate (0= constant value, 1= Ham (1958)) +1 # iNucleationRate (0= constant value, 1= Olander, Wongsawaeng (2006)) +1 # iOutput (1= default output files) +1 # iGrainBoundaryVacancyDiffusivity (0= constant value, 1= Reynolds and Burton (1979), 2= White (2004)) +1 # iGrainBoundaryBehaviour (0= no grain boundary bubbles, 1= Pastore et al (2013)) +1 # iGrainBoundaryMicroCracking (0= no model considered, 1= Barani et al. (2017)) +0 # iFuelMatrix (0= UO2, 1= UO2 + HBS) +0 # iGrainBoundaryVenting (0= no model considered, 1= Pizzocri et al., D6.4 (2020), H2020 Project INSPYRE) +0 # iRadioactiveFissionGas (0= not considered) +0 # iHelium (0= not considered) +0 # iHeDiffusivity (0= null value, 1= limited lattice damage, Luzzi et al. (2018), 2= significant lattice damage, Luzzi et al. (2018)) +0 # iGrainBoundarySweeping (0= no model considered, 1= TRANSURANUS swept volume model) +0 # iHighBurnupStructureFormation (0= no model considered, 1= fraction of HBS-restructured volume from Barani et al. (2020)) +0 # iHighBurnupStructurePorosity (0= no evolution of HBS porosity, 1= HBS porosity evolution based on Spino et al. (2006) data) +0 # iHeliumProductionRate (0= zero production rate, 1= helium from ternary fissions, 2= linear with burnup (FR)) +0 # iStoichiometryDeviation (0= not considered, 1= Cox et al. 1986, 2= Bittel et al. 1969, 3= Abrefah et al. 1994, 4= Imamura et al. 1997, 5= Langmuir-based approach) +0 # iBubbleDiffusivity (0= not considered, 1= volume diffusivity) \ No newline at end of file From f278fcbcad79502bab9a0df2c6e6a6fa8c72509a Mon Sep 17 00:00:00 2001 From: giozu Date: Wed, 18 Sep 2024 08:30:37 +0200 Subject: [PATCH 14/15] minor comments --- include/classes/Simulation.h | 24 ++++++++++++++++-------- 1 file changed, 16 insertions(+), 8 deletions(-) diff --git a/include/classes/Simulation.h b/include/classes/Simulation.h index f3aff192..27b61ec7 100644 --- a/include/classes/Simulation.h +++ b/include/classes/Simulation.h @@ -209,8 +209,7 @@ class Simulation void InterGranularBubbleBehavior(); /** - * @brief Calculates the sweeping of grain boundaries, particularly how it affects gas concentrations. - * Sweeping of the intra-granular gas concentrations. + * @brief Calculates the sweeping of grain boundaries, particularly how it affects intragranular gas concentrations. * * @author D. Pizzocri * @author T. Barani @@ -220,23 +219,32 @@ class Simulation void GrainBoundarySweeping(); /** - * @brief GrainBoundaryMicroCracking is method of simulation which executes - * the SCIANTIX simulation for the grain-boundary micro-cracking induced by a temperature difference. - * This method calls the related model "Grain-boundary micro-cracking", takes the model parameters and solve the model ODEs. + * @brief Calculates the fraction of cracked/healed grain-boundary faces after temperature transients, + * and the corresponding fission gas released. + * + * @author D. Pizzocri + * @author T. Barani + * @author G. Zullo + * */ void GrainBoundaryMicroCracking(); /** - * @brief Handles the venting processes at grain boundaries, potentially releasing gases. + * @brief Calculates the amount of gas released due to venting processes. + * + * @author D. Pizzocri + * @author T. Barani + * @author G. Zullo + * */ void GrainBoundaryVenting(); /** - * @brief Simulates the formation of high burnup structures within the nuclear fuel. + * @brief Calculates the formation of high burnup structures within the nuclear fuel. * + * @author G. Zullo * @author A. Magni * @author E. Redaelli - * @author G. Zullo * */ void HighBurnupStructureFormation(); From 2bba7e2fbe3cdd399bbb68ef2f46a99eb29f3883 Mon Sep 17 00:00:00 2001 From: giozu Date: Wed, 18 Sep 2024 08:38:26 +0200 Subject: [PATCH 15/15] use of action/upload-artifact@v4 --- .github/workflows/regression_test.yml | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/.github/workflows/regression_test.yml b/.github/workflows/regression_test.yml index 0f9cf410..cfc73f00 100644 --- a/.github/workflows/regression_test.yml +++ b/.github/workflows/regression_test.yml @@ -28,7 +28,7 @@ jobs: echo "in build" - name: Archive production artifacts - uses: actions/upload-artifact@v2 + uses: actions/upload-artifact@v4 with: name: compiled-build path: ./build @@ -40,7 +40,7 @@ jobs: steps: - uses: actions/checkout@v3 - name: Download build artifacts - uses: actions/download-artifact@v2 + uses: actions/download-artifact@v4 with: name: compiled-build path: ./build