]> https://gitweb.dealii.org/ - dealii.git/commitdiff
Use our ability to cross-link example programs.
authorWolfgang Bangerth <bangerth@math.tamu.edu>
Thu, 16 Mar 2006 16:31:18 +0000 (16:31 +0000)
committerWolfgang Bangerth <bangerth@math.tamu.edu>
Thu, 16 Mar 2006 16:31:18 +0000 (16:31 +0000)
git-svn-id: https://svn.dealii.org/trunk@12627 0785d39b-7218-0410-832d-ea1e28bc413d

deal.II/examples/step-12/step-12.cc

index adaf8bed6c47277a09b58e99816e4099a9a24cf6..0cdca96a4dd3522ab3ce173e92cfa238d9159b36 100644 (file)
@@ -549,7 +549,7 @@ void DGTransportEquation<dim>::assemble_face_term2(
                                 // proceed with the main part of this
                                 // program. The main class, here
                                 // called ``DGMethod'' is basically
-                                // the main class of step 6. One of
+                                // the main class of step-6. One of
                                 // the differences is that there's no
                                 // ConstraintMatrix object. This is,
                                 // because there are no hanging node
@@ -1473,13 +1473,13 @@ void DGMethod<dim>::solve (Vector<double> &solution)
                                 // that computes the approximate
                                 // gradients in a way similar to the
                                 // ``GradientEstimation'' described
-                                // in Step 9 of this tutorial. In
+                                // in step-9 of this tutorial. In
                                 // fact, the
                                 // ``DerivativeApproximation'' class
                                 // was developed following the
                                 // ``GradientEstimation'' class of
-                                // Step 9. Relating to the
-                                // discussion in Step 9, here we
+                                // step-9. Relating to the
+                                // discussion in step-9, here we
                                 // consider $h^{1+d/2}|\nabla_h
                                 // u_h|$. Futhermore we note that we
                                 // do not consider approximate second

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