diff options
author | jthorn <jthorn@e296648e-0e4f-0410-bd07-d597d9acff87> | 2002-05-13 16:17:42 +0000 |
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committer | jthorn <jthorn@e296648e-0e4f-0410-bd07-d597d9acff87> | 2002-05-13 16:17:42 +0000 |
commit | e0cabd60a58329a78fee053724a99a5cc11c05a0 (patch) | |
tree | da1e14b5a3a3e586e020e592a07422ff14677522 /doc | |
parent | 7adfaec40050e9ea3515fed55ec1643998adf6e3 (diff) |
add some clarifications suggested by Mitica Vulcanov
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinInitialData/Exact/trunk@68 e296648e-0e4f-0410-bd07-d597d9acff87
Diffstat (limited to 'doc')
-rw-r--r-- | doc/documentation.tex | 55 |
1 files changed, 35 insertions, 20 deletions
diff --git a/doc/documentation.tex b/doc/documentation.tex index a8c01ad..69ecd35 100644 --- a/doc/documentation.tex +++ b/doc/documentation.tex @@ -468,14 +468,15 @@ for each $i = 1$, $2$, $3$, $4$. \subsection{Pure-Radiation Robertson-Walker Cosmology} \verb|Exact::exactmodel = "Rob-Wal"| specifies a pure-radiation -Robertson-Walker spacetie ($p = \third \rho$, $k=0$), as described in +Robertson-Walker spacetime ($p = \third \rho$, $k=0$), as described in Hawking and Ellis section~5.3 and MTW section~27.11 (see also gr-qc/0110031), transformed to the usual Cactus $(t,x,y,z)$ Cartesian-topology coordinates. -The only physics parameter is -\begin{equation} -a = \text{\tt Desitt\_a} -\end{equation} -(note the name!). +The physics parameters are +\begin{align} +a &= \text{\tt Desitt\_a} \\ +b &= \text{\tt Desitt\_b} %%%\\ +\end{align} +(note the names!). The general Robertson-Walker line element in $(t,r,\theta,\phi)$ coordinates is @@ -490,7 +491,8 @@ ds^2 = -dt^2 + a t \left[ dr^2 + r^2 \, d\Omega^2 \right] This thorn also sets up the stress-energy tensor for this spacetime. -FIXME: more detail needed from Mitica +{\bf This solution doesn't work properly yet. See Mitica Vulcanov for +further information.} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% @@ -500,10 +502,12 @@ FIXME: more detail needed from Mitica spacetime (a zero-pressure spatially-flat Robertson-Walker spacetime), as described in Hawking and Ellis section~5.3 and MTW section~27.11 (see also gr-qc/0110031), transformed to the usual Cactus $(t,x,y,z)$ -Cartesian-topology coordinates. The only physics parameter is -\begin{equation} -a = \text{\tt Desitt\_a} -\end{equation} +Cartesian-topology coordinates. The physics parameters are +\begin{align} +a &= \text{\tt Desitt\_a} \\ +b &= \text{\tt Desitt\_b} %%%\\ +\end{align} +(note the name!). The Einstein-De~Sitter spacetime is the special case $R(t) = \sqrt{a}\,t^{2/3}$, $k = 0$ of the more general Robertson-Walker @@ -517,7 +521,8 @@ T_{tt} = \frac{1}{6 \pi t^2} \end{equation} This is properly set up by this thorn. -FIXME: more detail needed from Mitica +{\bf This solution doesn't work properly yet. See Mitica Vulcanov for +further information.} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% @@ -535,7 +540,8 @@ a = \text{\tt Godel\_a} At present this thorn doesn't set up the stress-energy tensor; you have to do this ``by hand''. -FIXME: more detail needed from Mitica +{\bf This solution doesn't work properly yet. See Mitica Vulcanov for +further information.} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% @@ -544,7 +550,11 @@ FIXME: more detail needed from Mitica \verb|Exact::exactmodel = "BianchiI"| specifies an approximation to a Bianchi type~I spacetime. -FIXME: more detail needed from Mitica +At present this thorn doesn't set up the stress-energy tensor; +you have to do this ``by hand''. + +{\bf This solution doesn't work properly yet. See Mitica Vulcanov for +further information.} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% @@ -584,15 +594,18 @@ T_{ab} = \diag \left[ \end{array} \right] \end{equation} -This is properly set up by this thorn. -FIXME: verify this with Mitica +{\bf At the moment only $T_{00}$ is set properly, the other +components are (incorrectly) 0. See Mitica Vulcanov for +further information.} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \subsection{Milne Spacetime for Pre-Big-Bang Cosmology} \verb|Exact::exactmodel = "Milne"| specifies a De~Milne spacetime, +as described by gr-qc/9802001 (see in particular reference~14, which +in turn points to Zeldovich and Novikov volume~2 section~2.4): \begin{equation} g_{ab} = \left[ \begin{array}{cccc} @@ -608,7 +621,8 @@ where V = \frac{t^2}{1 + x^2 + y^2 + z^2} \end{equation} -FIXME: more detail needed from Mitica +{\bf The $g_{ab}$ given here is indeed what the code computes, but +noone seems to know whether this is indeed a Milne (De~Milne?) spacetime.} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% @@ -632,9 +646,10 @@ tensor is also properly set up. \subsection{Non-Einstein Bowl (``Bag of Gold'') Spacetime} -\verb|Exact::exactmodel = "bowl"| specifies a ``bag of Gold'' metric. -This is useful for testing purposes, but isn't a solution of the -Einstein equations. The physics parameters are +\verb|Exact::exactmodel = "bowl"| specifies a ``bag of Gold'' metric, +as described in gr-qc/9809004. This is useful for testing purposes, +but isn't a solution of the Einstein equations. The physics parameters +are \begin{align} a & = \text{\tt bowl\_a} \\ \sigma & = \text{\tt bowl\_s} \\ |