From: bonito <bonito@0785d39b-7218-0410-832d-ea1e28bc413d>
Date: Wed, 5 Jan 2011 21:03:51 +0000 (+0000)
Subject: git-svn-id: https://svn.dealii.org/trunk@23131 0785d39b-7218-0410-832d-ea1e28bc413d
X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=b617f6790eb5c790c1d3a23d9f39b86047d2d88d;p=dealii-svn.git

git-svn-id: https://svn.dealii.org/trunk@23131 0785d39b-7218-0410-832d-ea1e28bc413d
---

diff --git a/deal.II/examples/step-38/doc/intro.dox b/deal.II/examples/step-38/doc/intro.dox
index f5145b3d4d..5008137e89 100644
--- a/deal.II/examples/step-38/doc/intro.dox
+++ b/deal.II/examples/step-38/doc/intro.dox
@@ -181,7 +181,7 @@ We produce one test case for a 2d problem and another one for 3d:
   In 3d, the domain is again half of the surface of the unit ball, i.e. a half
   sphere or dome. We choose $u(\mathbf x)=-2\sin(\pi x_1)\cos(\pi x_2)e^z$ as
   the solution. We can compute the right hand side of the
-  equation, $f=-\Delta_\Gamma u$, in the same way as the method above (in that case $\kappa = 2$), yielding an
+  equation, $f=-\Delta_\Gamma u$, in the same way as the method above (with $\kappa = 2$), yielding an
   awkward and lengthy expression. You can find the full expression in the
   source code.
 </li>