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authorhinder <hinder@8e189c6b-2ab8-4400-aa02-70a9cfce18b9>2011-10-25 12:38:10 +0000
committerhinder <hinder@8e189c6b-2ab8-4400-aa02-70a9cfce18b9>2011-10-25 12:38:10 +0000
commitd9e90b3e105b206a9802f63ee45512f6773cbe22 (patch)
treef283f36be297fe9e5d44431e0f9e96a62b40e56a
parente31cfbc5105a45c2333798ff3404e0447fd6387a (diff)
documentation.tex: Add braces for htlatex
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinEOS/EOS_Omni/trunk@51 8e189c6b-2ab8-4400-aa02-70a9cfce18b9
-rw-r--r--doc/documentation.tex10
1 files changed, 5 insertions, 5 deletions
diff --git a/doc/documentation.tex b/doc/documentation.tex
index c0b1f77..743c472 100644
--- a/doc/documentation.tex
+++ b/doc/documentation.tex
@@ -305,14 +305,14 @@ simulations of stellar collapse to mimic (1) the stiffening of the
nuclear EOS at nuclear density and (2) to include thermal pressure in
the postbounce phase. It consists of two polytropes characterized by
($K_1$, $\gamma_1$) and ($K_2$, $\gamma_2$) and a thermal $\gamma-$law
-component described by $\gamma_\mathrm{th}$. Polytrope 1 is soft and
+component described by $\gamma_{\mathrm{th}}$. Polytrope 1 is soft and
describes a gas of relativistic degenerate electrons with $\gamma_1
-\approx 4/3$. It is used below nuclear density ($\rho_\mathrm{nuc}
+\approx 4/3$. It is used below nuclear density ($\rho_{\mathrm{nuc}}
\approx 2\times10^{14}\,\mathrm{g\,cm}^{-3}$), and is smoothly matched to
-polytrope 2 which applies above $\rho_\mathrm{nuc}$, is stiff, and
+polytrope 2 which applies above $\rho_{\mathrm{nuc}}$, is stiff, and
models the repulsive core of the strong force above nuclear density
($\gamma_2 \gtrsim 2.5$). $K_2$ is completely determined by
-$P_1(\rho_\mathrm{nuc}) = P_2(\rho_\mathrm{nuc})$ and $K_1, \gamma_1,$
+$P_1(\rho_{\mathrm{nuc}}) = P_2(\rho_{\mathrm{nuc}})$ and $K_1, \gamma_1,$
and $\gamma_2$. The full functional form of the EOS
$P=P(\rho,\epsilon)$ with the thermal component (which takes into
account shock heating) is given by
@@ -331,7 +331,7 @@ The \texttt{EOS\_Omni} parameters for the hybrid EOS are the following:
\begin{tabular}{ll}
\texttt{hybrid\_gamma1} & $\gamma_1$, $\gamma_1 = 1.325$ is an appropriate choice.\\
\texttt{hybrid\_gamma2} & $\gamma_2$, $\gamma_2 = 2.5$ is an appropriate choice.\\
-\texttt{hybrid\_gamma\_th} & $\gamma_\mathrm{th}$, perhaps $1.5$.\\
+\texttt{hybrid\_gamma\_th} & $\gamma_{\mathrm{th}}$, perhaps $1.5$.\\
\texttt{hybrid\_k1} & $K_1$, $0.4640517$ in solar units for relativistic degenerate e$^{-}$.\\
\texttt{hybrid\_rho\_nuc} & nuclear density, standard is $3.238607\times 10^{-4}$ in solar units.
\end{tabular}