From: Felix Gruber Date: Mon, 12 Aug 2013 11:22:14 +0000 (+0000) Subject: Fix doxygen markup in documentation of step 51. X-Git-Tag: v8.1.0~1087 X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=0a77e0ea33aa9cf5757ef6b2eb73792689ec96d8;p=dealii.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 $\mathcal{O}(h^{p+2})$.

HDG applied to the convection-diffusion problem

The HDG formulation used for this example is taken from - +
N.C. Nguyen, J. Peraire, B. Cockburn: 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 $\{x_i\}_1^3 = \{ -\frac{1}{3}, 0, \frac{1}{3} \}$