% *======================================================================*
%  Cactus Thorn template for ThornGuide documentation
%  Author: Ian Kelley
%  Date: Sun Jun 02, 2002
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\documentclass{article}

% Use the Cactus ThornGuide style file
% (Automatically used from Cactus distribution, if you have a 
%  thorn without the Cactus Flesh download this from the Cactus
%  homepage at www.cactuscode.org)
\usepackage{../../../../doc/latex/cactus}

\begin{document}

% The author of the documentation
\author{Harry Dimmelmeier, Ian Hawke, Christian Ott} 

% The title of the document (not necessarily the name of the Thorn)
\title{EOS\_Hybrid}

% the date your document was last changed, if your document is in CVS, 
% please use:
\date{$ $Date$ $}

\maketitle

% Do not delete next line
% START CACTUS THORNGUIDE

% Add all definitions used in this documentation here 
%   \def\mydef etc

% Add an abstract for this thorn's documentation
\begin{abstract}
  EOS\_Hybrid. The equation of state used for ``simple'' core
  collapse simulations.
\end{abstract}

% The following sections are suggestive only.
% Remove them or add your own.

\section{The equations}
\label{sec:eqn}

This equation provides the hybrid polytropic / ideal gas equation of
state used by Dimmelmeier et al.~\cite{Dimm05} for supernova collapse. A thorn
wanting to use this needs to use the CactusEOS interface found in
EOS\_Base.

The equations are
\begin{eqnarray}
  \label{eq:eosformulas}
  P & = & P_{\textrm{poly}} + P_{\textrm{th}} \\
  \frac{\partial P}{\partial \rho} & = & \frac{\partial
  P_{\textrm{poly}}}{\partial \rho} + \frac{\partial
  P_{\textrm{th}_1}}{\partial \rho} + \frac{\partial
  P_{\textrm{th}_2}}{\partial \rho}  \\
  \frac{\partial P}{\partial \epsilon} & = & (\gamma_{\textrm{th}} - 1)
  \rho,
\end{eqnarray}
where
\begin{eqnarray}
  \label{eq:eostemps}
  P_{\textrm{poly}} & = & K \rho^{\gamma} \\
  P_{\textrm{th}} & = & -K \frac{\gamma_{\textrm{th}} - 1}{\gamma - 1}
  \rho^{\gamma} + (\gamma_{\textrm{th}} - 1) \rho \epsilon -
  (\gamma_{\textrm{th}} - 1) \frac{\gamma - \gamma_1}{\gamma_2 - 1} K
  \rho_{\textrm{nuc}}^{\gamma_1 - 1} \rho \\
  \frac{\partial P_{\textrm{poly}}}{\partial \rho} & = & \gamma K
  \rho^{\gamma - 1} \\ 
  \frac{\partial P_{\textrm{th}_1}}{\partial \rho} & = & - \gamma K
  \frac{\gamma_{\textrm{th}} - 1}{\gamma - 1} \rho^{\gamma -1} \\ 
  \frac{\partial P_{\textrm{th}_2}}{\partial \rho} & = & (\gamma - 1)
  \epsilon - (\gamma_{\textrm{th}} - 1) \frac{\gamma -
  \gamma_1}{(\gamma_1 - 1)(\gamma_2 - 1)} K \rho_{\textrm{nuc}}
  (\gamma_1 - 1).
\end{eqnarray}
These expressions do not include the conversions between cgs and
Cactus units that are necessary inside the code.

For more details, a recent paper to start with would
be~\cite{Dimm05}. 

% \section{Introduction}

% \section{Physical System}

% \section{Numerical Implementation}

% \section{Using This Thorn}

% \subsection{Obtaining This Thorn}

% \subsection{Basic Usage}

% \subsection{Special Behaviour}

% \subsection{Interaction With Other Thorns}

% \subsection{Support and Feedback}

% \section{History}

% \subsection{Thorn Source Code}

% \subsection{Thorn Documentation}

% \subsection{Acknowledgements}


\begin{thebibliography}{9}

\bibitem{Dimm05} 
H. Dimmelmeier, J. Novak, A. Font, J.~M. Ibanez, E. Mueller 
\newblock 
Combining spectral and shock-capturing methods: A new numerical approach 
for 3D relativistic core collapse simulations
\newblock Phys. Rev. D71 064023 (2005)

\end{thebibliography}

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\end{document}