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authorschnetter <schnetter@0cbbb82d-14ec-4423-a1fb-2ab18257ecaa>2004-01-17 12:46:11 +0000
committerschnetter <schnetter@0cbbb82d-14ec-4423-a1fb-2ab18257ecaa>2004-01-17 12:46:11 +0000
commit501b3bb424fd9ba19a00c4e20088a6407d25a3d1 (patch)
treede8788dd10476cb2c89913433e7ce1bf1179dc49
parent7d025c91fadf4003fbe88c350bfb55b3ef8e26b0 (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.tex4
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}]