]> https://gitweb.dealii.org/ - dealii-svn.git/commitdiff
git-svn-id: https://svn.dealii.org/trunk@23131 0785d39b-7218-0410-832d-ea1e28bc413d
authorbonito <bonito@0785d39b-7218-0410-832d-ea1e28bc413d>
Wed, 5 Jan 2011 21:03:51 +0000 (21:03 +0000)
committerbonito <bonito@0785d39b-7218-0410-832d-ea1e28bc413d>
Wed, 5 Jan 2011 21:03:51 +0000 (21:03 +0000)
deal.II/examples/step-38/doc/intro.dox

index f5145b3d4d6f8da6dc4a01e7d2f62183ea7c5d3d..5008137e894089f8d2628dbb799dc7294e0ff3f6 100644 (file)
@@ -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>

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