]> https://gitweb.dealii.org/ - dealii.git/commitdiff
Escape 'parallel'.
authorWolfgang Bangerth <bangerth@math.tamu.edu>
Wed, 23 Sep 2009 13:45:21 +0000 (13:45 +0000)
committerWolfgang Bangerth <bangerth@math.tamu.edu>
Wed, 23 Sep 2009 13:45:21 +0000 (13:45 +0000)
git-svn-id: https://svn.dealii.org/trunk@19504 0785d39b-7218-0410-832d-ea1e28bc413d

deal.II/examples/step-35/doc/intro.dox

index a79873627fcf9cc5f39647acc2fdeff2dcf0cda5..c32300af7b76af0c4955e30f003f226a60994246 100644 (file)
@@ -181,7 +181,7 @@ Moreover, to enforce the boundary condition on the pressure, we need to rewrite
 where the boundary integral in $\Gamma_1$ equals zero given the boundary conditions for the velocity,
 and the one in $\Gamma_2$ given the boundary conditions for the pressure.
 
-In the simplified case where the boundary $\Gamma_2$ is parallel to a coordinate axis, which holds for
+In the simplified case where the boundary $\Gamma_2$ is %parallel to a coordinate axis, which holds for
 the testcase that we carry out below, it can actually be shown that
 @f[
   \nu \int_\Omega \nabla u : \nabla v = \nu \int_\Omega \left[ \nabla \cdot u \nabla \cdot v

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