From: felix.gruber <felix.gruber@0785d39b-7218-0410-832d-ea1e28bc413d>
Date: Mon, 12 Aug 2013 11:22:14 +0000 (+0000)
Subject: Fix doxygen markup in documentation of step 51.
X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=8e5142e48394c13f1cfecd0851eee4f827e5f66f;p=dealii-svn.git

Fix doxygen markup in documentation of step 51.

git-svn-id: https://svn.dealii.org/trunk@30287 0785d39b-7218-0410-832d-ea1e28bc413d
---

diff --git a/deal.II/examples/step-51/doc/intro.dox b/deal.II/examples/step-51/doc/intro.dox
index 4ac27d1138..1bcbd31906 100644
--- a/deal.II/examples/step-51/doc/intro.dox
+++ b/deal.II/examples/step-51/doc/intro.dox
@@ -54,7 +54,7 @@ rate $\mathcal{O}(h^{p+2})$.
 <h3> HDG applied to the convection-diffusion problem </h3>
 
 The HDG formulation used for this example is taken from 
-<break>
+<br>
 <b>
   N.C. Nguyen, J. Peraire, B. Cockburn:
   <i>An implicit high-order hybridizable discontinuous Galerkin method 
@@ -88,11 +88,13 @@ the above equation as the first order system:
 Example specific data:
 $\Omega := [-1,1]^d$
 
+\f[
 \mathbf{c} = \begin{cases}
-1, & \textrm{dim}=1
-(y, -x), & \textrm{dim}=2
+1, & \textrm{dim}=1 \\
+(y, -x), & \textrm{dim}=2 \\
 (y, -x, 1), & \textrm{dim}=3
 \end{cases}
+\f]
 
 the centers $x_i$ of the exponentials are 
   $\{x_i\}_1^3 = \{ -\frac{1}{3}, 0, \frac{1}{3} \}$