diff options
author | schnetter <schnetter@0cbbb82d-14ec-4423-a1fb-2ab18257ecaa> | 2004-01-17 12:46:11 +0000 |
---|---|---|
committer | schnetter <schnetter@0cbbb82d-14ec-4423-a1fb-2ab18257ecaa> | 2004-01-17 12:46:11 +0000 |
commit | 501b3bb424fd9ba19a00c4e20088a6407d25a3d1 (patch) | |
tree | de8788dd10476cb2c89913433e7ce1bf1179dc49 | |
parent | 7d025c91fadf4003fbe88c350bfb55b3ef8e26b0 (diff) |
Fix typos
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinBase/StaticConformal/trunk@17 0cbbb82d-14ec-4423-a1fb-2ab18257ecaa
-rw-r--r-- | doc/documentation.tex | 4 |
1 files changed, 2 insertions, 2 deletions
diff --git a/doc/documentation.tex b/doc/documentation.tex index 9836da8..73b24c6 100644 --- a/doc/documentation.tex +++ b/doc/documentation.tex @@ -43,7 +43,7 @@ conformal\_storage} parameter. Note that the first and second ``derivative'' grid functions have an additional factor of $1 / \psi$ normalisation since this is the most -common use of the derivative. I.e. the grid functions are +common use of the derivative. I.e., the grid functions are \begin{eqnarray*} {\tt psi} &=& \psi, \\ @@ -58,7 +58,7 @@ actually been calculated before using the conformal factor: \begin{description} \item[{\tt conformal\_state=0}] No conformal factor has been calculated --- thorns may -assume the conformal factor is 1 at all points. (I.e. the metric is physical.) +assume the conformal factor is 1 at all points. (I.e., the metric is physical.) \item[{\tt conformal\_state=1}] The conformal factor has been calulated, but no derivatives. \item[{\tt conformal\_state=2}] |