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authoreschnett <eschnett@8e189c6b-2ab8-4400-aa02-70a9cfce18b9>2011-04-20 00:59:23 +0000
committereschnett <eschnett@8e189c6b-2ab8-4400-aa02-70a9cfce18b9>2011-04-20 00:59:23 +0000
commit16fb957603005e7dcc10a1864dcc2db7090ed8ba (patch)
treec077ccdaf17878c8340b376b4c782c298215e6bf
parentca8f2f01872319bb62037d81e70cea1a579c700d (diff)
Some grammar corrections
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinEOS/EOS_Omni/trunk@46 8e189c6b-2ab8-4400-aa02-70a9cfce18b9
-rw-r--r--doc/documentation.tex16
1 files changed, 8 insertions, 8 deletions
diff --git a/doc/documentation.tex b/doc/documentation.tex
index 55b9e94..416f59c 100644
--- a/doc/documentation.tex
+++ b/doc/documentation.tex
@@ -112,11 +112,11 @@ Erik Schnetter \textless eschnetter@perimeterinstitute.ca\textgreater}
\begin{abstract}
\noindent This thorn provides a unified EOS (Equation Of State)
- interface and implements multiple analytic EOS and provides table
+ interface and implements multiple analytic EOS, and also provides table
reader and interpolation routines for finite-temperature
- microphysical EOS available from {\tt
- http://www.stellarcollapse.org}\@. Currently, the implemented
- analytic EOS are the polytropic EOS, the gamma-law EOS, a hybrid EOS
+ microphysical EOS available from
+ \url{http://www.stellarcollapse.org}. Currently, the implemented
+ analytic EOS are the polytropic EOS, the gamma-law EOS, and a hybrid EOS
consisting of a 2-piece piecewise-polytrope with an a thermal,
gamma-law component.
\end{abstract}
@@ -150,7 +150,7 @@ Temperatures are measured in MeV.
\texttt{EOS\_Omni} works via the aliased-function interface, and
EOS functions to be used must be declared in \texttt{interface.ccl}.
-Here is an example call/{interface.ccl} entry:
+Here is an example \texttt{interface.ccl} entry:
\begin{verbatim}
void FUNCTION EOS_Omni_press(CCTK_INT IN eoskey, \
CCTK_INT IN havetemp, \
@@ -176,7 +176,7 @@ Here,
\item \texttt{eoskey = 4}: Finite-temperature microphysical EOS
\end{itemize}
\item \texttt{havetemp} determines whether the EOS is to be called as
- a function of $(\rho,\epsilon,Y_e)$ (\texttt{havetemp = 0}), as a
+ a function of $(\rho,\epsilon,Y_e)$ (\texttt{havetemp = 0}), or as a
function of $(\rho,T,Y_e)$ (\texttt{havetemp = 1}).
\texttt{havetemp = 0} is the method of choice for analytic EOS during
evolution, but at the initial data stage one may need to set
@@ -249,7 +249,7 @@ relation
\end{eqnarray}
(which actually ignores the temperature).
-Internally, \texttt{EOS\_Omni} uses cgs units and on startup converts
+Internally, \texttt{EOS\_Omni} uses cgs units, and on startup converts
the EOS parameters from solar units to cgs units. This conversion
depends on $\gamma$ and the value of $\gamma$ at the initial
data stage (\texttt{poly\_gamma\_ini}) is used for this.
@@ -310,7 +310,7 @@ the postbounce phase. It consists of two polytropes characterized by
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 ($\rho_\mathrm{nuc}
-\approx 2\times10^{14}\,\mathrm{g\,cm}^{-3}$) and smoothly matched to
+\approx 2\times10^{14}\,\mathrm{g\,cm}^{-3}$), and is smoothly matched to
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