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diff --git a/Master/texmf-dist/doc/latex/nomencl/sample03.tex b/Master/texmf-dist/doc/latex/nomencl/sample03.tex new file mode 100644 index 00000000000..f06ad3f196b --- /dev/null +++ b/Master/texmf-dist/doc/latex/nomencl/sample03.tex @@ -0,0 +1,37 @@ +\documentclass{article} +\usepackage[nomentbl,stdsubgroups]{nomencl} +\usepackage{setspace} +\makenomenclature +\begin{document} +\section*{Main equations} +Here an equation + \begin{equation}\label{eq:heatflux} + \dot{Q} = k \cdot A \cdot \Delta T + \end{equation}% + \nomenclature[aQ]{$\dot{Q}$}{heat flux}{W}{}% + \nomenclature[ak]{$k$}{overall heat transfer + coefficient}{\watt\per(\square\meter\kelvin)}{see + eq.~(\ref{eq:ohtc})}% + \nomenclature[aA]{$A$}{area}{\square\meter}{}% + \nomenclature[aL]{$L$}{length}{\meter}{SI base quantity}% + \nomenclature[aT]{$T$}{temperature}{\kelvin}{SI base quantity}% + \nomenclature[aT]{$\Delta T$}{temperature difference}{\kelvin}{SI base quantity}% +or another one + \begin{equation}\label{eq:ohtc} + \frac{1}{k} = \left[\frac{1}{\alpha _{\mathrm{i}}\,r_{\mathrm{i}}} + + \sum^n_{j=1}\frac{1}{\lambda _j}\, + \ln \frac{r_{\mathrm{a},j}}{r_{\mathrm{i},j}} + + \frac{1}{\alpha _{\mathrm{a}}\, + r_{\mathrm{a}}}\right] \cdot r_{\mathrm{reference}} + \end{equation}% + \nomenclature[ga]{$\alpha$}{convection heat transfer + coefficient}{\watt\per(\square\meter\kelvin)}{}% + \nomenclature[zi]{i}{in}{}{}% + \nomenclature[gl]{$\lambda$}{thermal conductivity}{\watt\per\kelvin}{}% + \nomenclature[za]{a}{out}{}{}% + \nomenclature[zn]{$n$}{number of walls}{}{}% + \nomenclature[zj]{$j$}{running parameter}{}{}% + +\onehalfspacing +\printnomenclature +\end{document} |