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maxdepth: 2 | ||
chapters: | ||
- file: installation | ||
- file: examples |
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(examples)= | ||
# Examples | ||
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```{contents} | ||
:local: | ||
``` | ||
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```{tableofcontents} | ||
``` |
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# Installation | ||
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The implementation is based on the high-order finite element library [NGSolve](https://ngsolve.org) which can be installed using | ||
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``` | ||
python -m pip install numpy scipy matplotlib jupyter ipyparallel scikit-build | ||
python -m pip install --upgrade ngsolve webgui_jupyter_widgets | ||
``` | ||
For troubleshooting and more details on the installation we refer to the various `NGSolve` installation tutorials [NGS24](https://docu.ngsolve.org/ngs24/intro.html) or the [NGSolve Documentation](https://docu.ngsolve.org/latest/). | ||
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To run the `*.ipynb` examples you additionally need an installation of [jupyter](https://jupyter.org/install) |
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\documentclass[border=1mm]{standalone} | ||
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\usepackage[utf8]{inputenc} | ||
\usepackage[T1]{fontenc} | ||
\usepackage[english]{babel} | ||
\usepackage{graphicx} | ||
\usepackage{xcolor} | ||
\usepackage{tikz} | ||
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%%%%%emph colors | ||
\definecolor{emph1}{RGB}{0,102,153} | ||
\definecolor{emph2}{RGB}{200,90,20} | ||
\definecolor{emph3}{RGB}{100,30,153} | ||
\definecolor{emph4}{RGB}{0,100,0} | ||
\definecolor{emph5}{RGB}{0,100,200} | ||
\definecolor{emph6}{RGB}{100,0,0} | ||
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\begin{document} | ||
\begin{tikzpicture} | ||
\node[black, opacity=0.2] at (3.7,-3.2){\resizebox{!}{100pt}{$\partial_t$}}; | ||
\node[emph1, opacity=0.8] at (3.5,-3){\resizebox{!}{100pt}{$\partial_t$}}; | ||
\node[black, opacity=0.2] at (0.2,-0.2){\resizebox{!}{100pt}{$-i\omega$}}; | ||
\node[emph2, opacity=0.8] at (0,0){\resizebox{!}{100pt}{$-i\omega$}}; | ||
\end{tikzpicture} | ||
\end{document} |
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@article{WKCS2023, | ||
title = {Mass lumping the dual cell method to arbitrary polynomial degree for acoustic and electromagnetic waves}, | ||
journal = {Journal of Computational Physics}, | ||
pages = {113196}, | ||
year = {2024}, | ||
issn = {0021-9991}, | ||
doi = {https://doi.org/10.1016/j.jcp.2024.113196}, | ||
urlremoved = {https://www.sciencedirect.com/science/article/pii/S0021999124004455}, | ||
author = {Markus Wess and Bernard Kapidani and Lorenzo Codecasa and Joachim Schöberl}, | ||
keywords = {Time-Domain Maxwell Equations, Cell Method, Discontinuous Galerkin, Dual Grids, Mass Lumping, High-Order Finite Elements}, | ||
abstract = {We present a fundamental improvement of a high polynomial degree time domain cell method recently introduced by the last three authors. The published work introduced a method featuring block-diagonal system matrices where the block size and conditioning scaled poorly with respect to polynomial degree. The issue is herein bypassed by the construction of new basis functions exploiting quadrature rule based mass lumping techniques for arbitrary polynomial degrees in two dimensions for the Maxwell equations and the acoustic wave equation in the first order velocity pressure formulation. We characterize the degrees of freedom of all new discrete approximation spaces we employ for differential forms and show that the resulting block diagonal (inverse) mass matrices have block sizes independent of the polynomial degree. We demonstrate on an extensive number of examples how the new technique is applicable and efficient for large scale computations.} | ||
} | ||
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@article {KCS2021, | ||
AUTHOR = {Kapidani, Bernard and Codecasa, Lorenzo and Sch\"{o}berl, | ||
Joachim}, | ||
TITLE = {An arbitrary-order cell method with block-diagonal | ||
mass-matrices for the time-dependent 2{D} {M}axwell equations}, | ||
JOURNAL = {J. Comput. Phys.}, | ||
FJOURNAL = {Journal of Computational Physics}, | ||
VOLUME = {433}, | ||
YEAR = {2021}, | ||
PAGES = {Paper No. 110184, 20}, | ||
ISSN = {0021-9991,1090-2716}, | ||
MRCLASS = {65M60 (78M10)}, | ||
MRNUMBER = {4216954}, | ||
MRREVIEWER = {Jinbiao\ Wu}, | ||
DOI = {10.1016/j.jcp.2021.110184}, | ||
URLREMOVED = {https://doi.org/10.1016/j.jcp.2021.110184}, | ||
} | ||
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@article{Stolk, | ||
author = {Stolk, Christiaan C.}, | ||
title = {A Time-Domain Preconditioner for the Helmholtz Equation}, | ||
journal = {SIAM Journal on Scientific Computing}, | ||
volume = {43}, | ||
number = {5}, | ||
pages = {A3469-A3502}, | ||
year = {2021}, | ||
doi = {10.1137/20M1359997}, | ||
} | ||
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@article{AGFR, | ||
author = {Appel\"{o}, Daniel and Garcia, Fortino and Runborg, Olof}, | ||
title = {WaveHoltz: Iterative Solution of the Helmholtz Equation via the Wave Equation}, | ||
journal = {SIAM Journal on Scientific Computing}, | ||
volume = {42}, | ||
number = {4}, | ||
pages = {A1950-A1983}, | ||
year = {2020}, | ||
doi = {10.1137/19M1299062}, | ||
} | ||
@misc{nw24, | ||
@misc{NW24, | ||
title={A Krylov Eigenvalue Solver Based on Filtered Time Domain Solutions}, | ||
author={Lothar Nannen and Markus Wess}, | ||
year={2024}, | ||
eprint={2402.08515}, | ||
archivePrefix={arXiv}, | ||
primaryClass={id='math.NA' full_name='Numerical Analysis' is_active=True alt_name='cs.NA' in_archive='math' is_general=False description='Numerical algorithms for problems in analysis and algebra, scientific computation'} | ||
} | ||
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@article{Knyazev, | ||
author = {Knyazev, Andrew V.}, | ||
title = {Toward the Optimal Preconditioned Eigensolver: Locally Optimal Block Preconditioned Conjugate Gradient Method}, | ||
journal = {SIAM Journal on Scientific Computing}, | ||
volume = {23}, | ||
number = {2}, | ||
pages = {517-541}, | ||
year = {2001}, | ||
doi = {10.1137/S1064827500366124}, | ||
} |