From: Andrea Bonito 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-Tag: v8.0.0~4528 X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=d48ff985dce19f79f6fb4855e99075e63bcef391;p=dealii.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.