From b617f6790eb5c790c1d3a23d9f39b86047d2d88d Mon Sep 17 00:00:00 2001 From: bonito Date: Wed, 5 Jan 2011 21:03:51 +0000 Subject: [PATCH] git-svn-id: https://svn.dealii.org/trunk@23131 0785d39b-7218-0410-832d-ea1e28bc413d --- deal.II/examples/step-38/doc/intro.dox | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) 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. -- 2.39.5