]> https://gitweb.dealii.org/ - dealii.git/commitdiff
Tweak some example documentation.
authorDavid Wells <drwells@email.unc.edu>
Thu, 22 Jun 2023 03:16:11 +0000 (23:16 -0400)
committerDavid Wells <drwells@email.unc.edu>
Thu, 22 Jun 2023 03:16:11 +0000 (23:16 -0400)
examples/step-15/step-15.cc
examples/step-36/doc/intro.dox
examples/step-39/doc/results.dox
examples/step-7/doc/results.dox

index c10aabf064fe6290d1b28dc780bb7006d0e29f32..30ccc56a8dee0c1f7242f17c1e9512ebbc63baec 100644 (file)
@@ -683,7 +683,7 @@ namespace Step15
         ++refinement_cycle;
         std::cout << std::endl;
       }
-    while (last_residual_norm > 1e-3);
+    while (last_residual_norm > 1e-2);
   }
 } // namespace Step15
 
index 085bf3d7e97ce6ec29a2d6ba0058c2f494840ce2..92816cefbe8b8d3b52e3075ce1e0c970a646f05e 100644 (file)
@@ -18,9 +18,8 @@ course equally applicable to the other applications above.
 
 Eigenspectrum problems have the general form
 @f{align*}
-       L \Psi &= \varepsilon \Psi \qquad &&\text{in}\ \Omega\quad,
-       \\
-       \Psi &= 0 &&\text{on}\ \partial\Omega\quad,
+    L \Psi &= \varepsilon \Psi \qquad &&\text{in}\ \Omega, \\
+    \Psi   &= 0 &&\text{on}\ \partial\Omega,
 @f}
 where the Dirichlet boundary condition on $\Psi=\Psi(\mathbf x)$ could also be
 replaced by Neumann or Robin conditions; $L$ is an operator that generally
index c3531d9d4b8b977330c60e422a9a7383b5a5b0f8..25a47ac4dacdaccf5ea9b60671bdf35eb606e064 100644 (file)
@@ -91,7 +91,7 @@ data into <tt>output.dat</tt>, which can be used to plot graphs with
 script <tt>plot_errors.gpl</tt> via
 
 @code
-perl postprocess.pl deallog &> output.dat
+./step-39 | perl postprocess.pl >output.dat
 gnuplot plot_errors.gpl
 @endcode
 
index ae5a4c9f9c30275c2a30f68e056be01bf8c612b5..de8f65c895602ff23b406f9922f0fbf3cee2e3ee 100644 (file)
@@ -15,7 +15,7 @@ here:
 
 Secondly, the program writes tables not only to disk, but also to the
 screen while running. The output looks like the following (recall that
-columns labeled as "<code>H1</code>" actually show the $H^1$ <i>semi-</i>norm
+columns labeled as "H1" actually show the $H^1$ <i>semi-</i>norm
 of the error, not the full $H^1$ norm):
 
 

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