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function toggleVisibility(linkObj) | ||
{ | ||
var base = $(linkObj).attr('id'); | ||
var summary = $('#'+base+'-summary'); | ||
var content = $('#'+base+'-content'); | ||
var trigger = $('#'+base+'-trigger'); | ||
var src=$(trigger).attr('src'); | ||
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content.hide(); | ||
summary.show(); | ||
$(linkObj).addClass('closed').removeClass('opened'); | ||
$(trigger).attr('src',src.substring(0,src.length-8)+'closed.png'); | ||
} else { | ||
content.show(); | ||
summary.hide(); | ||
$(linkObj).removeClass('closed').addClass('opened'); | ||
$(trigger).attr('src',src.substring(0,src.length-10)+'open.png'); | ||
} | ||
return false; | ||
} | ||
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function updateStripes() | ||
{ | ||
$('table.directory tr'). | ||
removeClass('even').filter(':visible:even').addClass('even'); | ||
} | ||
function toggleLevel(level) | ||
{ | ||
$('table.directory tr').each(function(){ | ||
var l = this.id.split('_').length-1; | ||
var i = $('#img'+this.id.substring(3)); | ||
var a = $('#arr'+this.id.substring(3)); | ||
if (l<level+1) { | ||
i.attr('src','ftv2folderopen.png'); | ||
a.attr('src','ftv2mnode.png'); | ||
$(this).show(); | ||
} else if (l==level+1) { | ||
i.attr('src','ftv2folderclosed.png'); | ||
a.attr('src','ftv2pnode.png'); | ||
$(this).show(); | ||
} else { | ||
$(this).hide(); | ||
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updateStripes(); | ||
} | ||
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function toggleFolder(id) | ||
{ | ||
//The clicked row | ||
var currentRow = $('#row_'+id); | ||
var currentRowImages = currentRow.find("img"); | ||
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//All rows after the clicked row | ||
var rows = currentRow.nextAll("tr"); | ||
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//Only match elements AFTER this one (can't hide elements before) | ||
var childRows = rows.filter(function() { | ||
var re = new RegExp('^row_'+id+'\\d+_$', "i"); //only one sub | ||
return this.id.match(re); | ||
}); | ||
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||
//First row is visible we are HIDING | ||
if (childRows.filter(':first').is(':visible')===true) { | ||
currentRowImages.filter("[id^=arr]").attr('src', 'ftv2pnode.png'); | ||
currentRowImages.filter("[id^=img]").attr('src', 'ftv2folderclosed.png'); | ||
rows.filter("[id^=row_"+id+"]").hide(); | ||
} else { //We are SHOWING | ||
//All sub images | ||
var childImages = childRows.find("img"); | ||
var childImg = childImages.filter("[id^=img]"); | ||
var childArr = childImages.filter("[id^=arr]"); | ||
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||
currentRow.find("[id^=arr]").attr('src', 'ftv2mnode.png'); //open row | ||
currentRow.find("[id^=img]").attr('src', 'ftv2folderopen.png'); //open row | ||
childImg.attr('src','ftv2folderclosed.png'); //children closed | ||
childArr.attr('src','ftv2pnode.png'); //children closed | ||
childRows.show(); //show all children | ||
} | ||
updateStripes(); | ||
} | ||
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function toggleInherit(id) | ||
{ | ||
var rows = $('tr.inherit.'+id); | ||
var img = $('tr.inherit_header.'+id+' img'); | ||
var src = $(img).attr('src'); | ||
if (rows.filter(':first').is(':visible')===true) { | ||
rows.css('display','none'); | ||
$(img).attr('src',src.substring(0,src.length-8)+'closed.png'); | ||
} else { | ||
rows.css('display','table-row'); // using show() causes jump in firefox | ||
$(img).attr('src',src.substring(0,src.length-10)+'open.png'); | ||
} | ||
} | ||
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\form#0:$\overline{g}$ | ||
\form#1:$\textrm{K}$ | ||
\form#2:$\textrm{K}_\mathrm{col}$ | ||
\form#3:$\overline{\mu}_\mathrm{tr}/\rho$ | ||
\form#4:$\overline{\mu}_\mathrm{en}/\rho$ | ||
\form#5:$\mu_\mathrm{en}$ | ||
\form#6:$\mu_\mathrm{en}/\rho$ | ||
\form#7:$\mu_\mathrm{tr}/\rho$ | ||
\form#8:$\sigma$ | ||
\form#9:$T_0$ | ||
\form#10:$\overline{E}_\mathrm{rad}$ | ||
\form#11:\begin{equation} Y = \frac{\overline{E}_\mathrm{rad}}{T_0}. \end{equation} | ||
\form#12:$Y_\mathrm{brems}$ | ||
\form#13:$\overline{E}_\mathrm{tot}$ | ||
\form#14:$T(E)$ | ||
\form#15:$\overline{T}$ | ||
\form#16:\begin{equation}\label{def_mutr} \left(\frac{\mu_\mathrm{tr}}{\rho}\right) = \frac{\overline{E}_\mathrm{tr}}{E} \cdot \left(\frac{\mu}{\rho}\right), \end{equation} | ||
\form#17:$\overline{E}_\mathrm{tr}$ | ||
\form#18:$\mu/\rho$ | ||
\form#19:\begin{equation}\label{def_muen} \left(\frac{\mu_\mathrm{en}}{\rho}\right) = \left(1-\overline{g}\right) \cdot \left(\frac{\mu_\mathrm{tr}}{\rho}\right) = \frac{\overline{E}_\mathrm{ab}}{E} \cdot \left(\frac{\mu}{\rho}\right), \end{equation} | ||
\form#20:$\overline{E}_\mathrm{ab}$ | ||
\form#21:$\overline{\overline{E}}_\mathrm{rad}$ | ||
\form#22:\begin{equation}\label{eq_g_mono} \overline{g} = \frac{\overline{\overline{E}}_\mathrm{rad}}{\overline{E}_\mathrm{tr}}, \end{equation} | ||
\form#23:\begin{equation}\label{EradP} \overline{\overline{E}}_\mathrm{rad} = \overline{E}_\mathrm{tr} - \overline{E}_\mathrm{ab}. \end{equation} | ||
\form#24:\begin{equation}\label{eq:K} \frac{K}{\phi} = E \cdot \left(\mu_\mathrm{tr}/\rho\right), \end{equation} | ||
\form#25:\begin{equation}\label{eq:Kcol} \frac{K_\mathrm{col}}{\phi} = E \cdot \left(\mu_\mathrm{en}/\rho\right). \end{equation} | ||
\form#26:\begin{equation}\label{eq:def} \frac{K}{\phi} = \int \phi(E) \cdot E \cdot \left[\frac{\mu_\mathrm{tr}(E)}{\rho}\right] \cdot dE/\int \phi(E) \cdot dE. \end{equation} | ||
\form#27:\begin{equation}\label{eq:Kpoly} \frac{K}{\phi} = \left<\mu_\mathrm{tr}/\rho\right>_{\psi} \cdot \left<E\right>_{\phi} = \left<E\cdot\mu_\mathrm{tr}/\rho\right>_{\phi}. \end{equation} | ||
\form#28:$\mu_\mathrm{tr}$ | ||
\form#29:\begin{equation}\label{eq:Kpolycol}\label{eq_kerma_0} \frac{K_\mathrm{col}}{\phi} = \left<\mu_\mathrm{en}/\rho\right>_{\psi} \cdot \left<E\right>_{\phi} = \left<E\cdot\mu_\mathrm{en}/\rho\right>_{\phi}. \end{equation} | ||
\form#30:\begin{equation}\label{eq_kerma_1} \frac{K_\mathrm{col}}{\phi} = \left(1-\overline{g}\right) \frac{K}{\phi} = \left(1-\overline{g}\right) \left<E\cdot\mu_\mathrm{tr}/\rho\right>_{\phi}, \end{equation} | ||
\form#31:\begin{equation} \overline{g} = 1 - \frac{\left<E\cdot\mu_\mathrm{en}\right>_{\phi}}{\left<E\cdot\mu_\mathrm{tr}\right>_{\phi}}, \end{equation} | ||
\form#32:\begin{equation}\label{eq:g} \overline{g} = 1 - \frac{\left<\overline{E}_\mathrm{en}\cdot\mu\right>_{\phi}}{\left<\overline{E}_\mathrm{tr}\cdot\mu\right>_{\phi}} = \frac{\left<\overline{\overline{E}}_\mathrm{rad}\cdot\mu\right>_{\phi}}{\left<\overline{E}_\mathrm{tr}\cdot\mu\right>_{\phi}} \end{equation} | ||
\form#33:$\left<\mu_\mathrm{tr}/\rho\right>_{\psi}$ | ||
\form#34:\begin{equation} \left<\mu_\mathrm{tr}/\rho\right>_{\psi} = \frac{\left<E\cdot\mu_\mathrm{tr}/\rho\right>_{\phi}}{\left<E\right>_{\phi}} = \frac{\left<\overline{E}_\mathrm{tr}\cdot\mu\right>_{\phi}}{\left<E\right>_{\phi}}, \end{equation} | ||
\form#35:$\left<\mu_\mathrm{en}/\rho\right>_{\psi}$ | ||
\form#36:\begin{equation}\label{eq_muen_0} \left<\mu_\mathrm{en}/\rho\right>_{\psi} = \frac{\left<E\cdot\mu_\mathrm{en}/\rho\right>_{\phi}}{\left<E\right>_{\phi}} = \frac{\left<\overline{E}_\mathrm{en}\cdot\mu\right>_{\phi}}{\left<E\right>_{\phi}}, \end{equation} | ||
\form#37:\begin{equation}\label{eq_muen_1} \left<\mu_\mathrm{en}/\rho\right>_{\psi} = \left(1-\overline{g}\right) \left<\mu_\mathrm{tr}/\rho\right>_{\psi}, \end{equation} | ||
\form#38:$\sigma/\sqrt{4/3}$ | ||
\form#39:$\sigma/2$ | ||
\form#40:$E$ | ||
\form#41:$q$ | ||
\form#42:$\Delta\mathrm{E}$ | ||
\form#43:$E_\mathrm{min}, ..., E_\mathrm{min} + i \cdot \Delta\mathrm{E}, ..., E_\mathrm{max}$ | ||
\form#44:$\Delta_\mathrm{log}$ | ||
\form#45:\begin{equation} \Delta_\mathrm{log} = log\left(\frac{E_\mathrm{max}}{E_\mathrm{min}}\right)/\left(N-1\right) \end{equation} | ||
\form#46:\begin{equation} E_i = e^{log(E_\mathrm{min})+i \cdot \Delta_\mathrm{log}} \end{equation} | ||
\form#47:\begin{equation} \sigma(\mu_\mathrm{tr}) = \frac{\sigma}{\sqrt{m}} \qquad \textrm{and} \qquad \sigma(1-\overline{g}) = \frac{\sigma}{\sqrt{m/(m-1)}} \end{equation} |
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 <span id="projectnumber">Report PIRS-3100</span> | ||
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<div class="textblock"><p>Documents the g application. </p> | ||
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