]> https://gitweb.dealii.org/ - dealii-svn.git/commitdiff
Fix a typo in the documentation of step-52.
authorturcksin <turcksin@0785d39b-7218-0410-832d-ea1e28bc413d>
Tue, 20 May 2014 22:48:16 +0000 (22:48 +0000)
committerturcksin <turcksin@0785d39b-7218-0410-832d-ea1e28bc413d>
Tue, 20 May 2014 22:48:16 +0000 (22:48 +0000)
git-svn-id: https://svn.dealii.org/trunk@32951 0785d39b-7218-0410-832d-ea1e28bc413d

deal.II/examples/step-52/doc/intro.dox

index e2706e98ebf2123a5122819590ec9ae3e820b310..ac7c4e03298875dcb96257d3993d662121372f35 100644 (file)
@@ -23,7 +23,7 @@ neutrons, $D$ is the diffusion coefficient, $\Sigma_a$ is the <i>absorption
 cross section</i>, and $S$ is a source. Because we are only interested in the
 time dependence, we assume that $D$ and $\Sigma_a$ are constant. In this
 example, we are only interested in the error in time. The domain is square
-$[0,b]\times[0,b] and we are looking for a solution of the form:
+$[0,b]\times[0,b]$ and we are looking for a solution of the form:
 @f{eqnarray*}
 \phi(x,t) = A\sin(\omega t)(bx-x^2).
 @f}

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