From: kanschat
Date: Wed, 29 Aug 2007 14:59:45 +0000 (+0000)
Subject: remove html warnings and errors
X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=dff5900fde2fa8517cdd9d37a2e6e617284327f6;p=dealii-svn.git
remove html warnings and errors
git-svn-id: https://svn.dealii.org/trunk@15085 0785d39b-7218-0410-832d-ea1e28bc413d
---
diff --git a/deal.II/doc/development/index.html b/deal.II/doc/development/index.html
index 81ab38694b..78c4491ef8 100644
--- a/deal.II/doc/development/index.html
+++ b/deal.II/doc/development/index.html
@@ -3,10 +3,10 @@
deal.II Development Information
-
+
-
+
diff --git a/deal.II/doc/documentation.html b/deal.II/doc/documentation.html
index eb758fc245..12103f801d 100644
--- a/deal.II/doc/documentation.html
+++ b/deal.II/doc/documentation.html
@@ -2,7 +2,7 @@
"http://www.w3.org/TR/html4/loose.dtd">
-
+
The deal.II Online Documentation
@@ -63,7 +63,7 @@
The documentation uses many of the features of Doxygen. In particular,
- the link takes you straight to a page that lists modules, a way
+ the link takes you straight to a page that lists modules, a way
to group classes with similar purposes. This may be what you are probably
interested in when you are not yet familiar with the library. If you
already know your way around and want to look up the signature of a
diff --git a/deal.II/doc/doxygen/tutorial/index.html b/deal.II/doc/doxygen/tutorial/index.html
index 9f5ca82047..e34c6af7be 100644
--- a/deal.II/doc/doxygen/tutorial/index.html
+++ b/deal.II/doc/doxygen/tutorial/index.html
@@ -7,19 +7,14 @@
-->
Step-by-Step Examples
-
+
-
Introduction:A brief description of what the program does and
what is new compared to the previous programs. This also includes a
@@ -38,7 +36,6 @@ follows:
program again, with all comments stripped off, to allow getting an
overview of it.
-
The programs can be found at a path which is indicated at
@@ -52,7 +49,7 @@ in in this section.
The program has, after having been run, produced two grids, which look
diff --git a/deal.II/examples/step-10/doc/results.dox b/deal.II/examples/step-10/doc/results.dox
index cccf2683e5..84d1954b6e 100644
--- a/deal.II/examples/step-10/doc/results.dox
+++ b/deal.II/examples/step-10/doc/results.dox
@@ -1,4 +1,3 @@
-
This is what the program outputs:
diff --git a/deal.II/examples/step-12/doc/results.dox b/deal.II/examples/step-12/doc/results.dox
index 63ff406f6f..2ca9f6b9d6 100644
--- a/deal.II/examples/step-12/doc/results.dox
+++ b/deal.II/examples/step-12/doc/results.dox
@@ -1,4 +1,3 @@
-
The program has, after having been run, produced two sparsity
diff --git a/deal.II/examples/step-20/doc/results.dox b/deal.II/examples/step-20/doc/results.dox
index e0f4f0334d..94d37d19e0 100644
--- a/deal.II/examples/step-20/doc/results.dox
+++ b/deal.II/examples/step-20/doc/results.dox
@@ -1,4 +1,3 @@
-
If we run the program, we get the following kind of output:
@code
diff --git a/deal.II/examples/step-23/doc/results.dox b/deal.II/examples/step-23/doc/results.dox
index 205a2cc6eb..1540a35ba7 100644
--- a/deal.II/examples/step-23/doc/results.dox
+++ b/deal.II/examples/step-23/doc/results.dox
@@ -1,4 +1,3 @@
-
Results
When the program is run, it produces the following output:
diff --git a/deal.II/examples/step-24/doc/results.dox b/deal.II/examples/step-24/doc/results.dox
index 25d2d15f74..25cc204f3d 100644
--- a/deal.II/examples/step-24/doc/results.dox
+++ b/deal.II/examples/step-24/doc/results.dox
@@ -1,4 +1,3 @@
-
Results
The program writes both graphical data for each time step as well as the
diff --git a/deal.II/examples/step-25/doc/results.dox b/deal.II/examples/step-25/doc/results.dox
index 0cabb43857..aebb044ac6 100644
--- a/deal.II/examples/step-25/doc/results.dox
+++ b/deal.II/examples/step-25/doc/results.dox
@@ -1,4 +1,4 @@
-
Results
+
Results
The explicit Euler time stepping scheme ($\theta=0$) performs adequately for the problems we wish to solve. Unfortunately, a rather small time step has to be chosen due to stability issues --- $k\sim h/10$ appears to work for most the simulations we performed. On the other hand, the Crank-Nicolson scheme ($\theta=\frac{1}{2}$) is unconditionally stable, and (at least for the case of the 1D breather) we can pick the time step to be as large as $25h$ without any ill effects on the solution. The implicit Euler scheme ($\theta=1$) is "exponentially damped," so it is not a good choice for solving the sine-Gordon equation, which is conservative. However, some of the damped schemes in the continuum that is offered by the $\theta$-method were useful for eliminating spurious oscillations due to boundary effects.
In the simulations below, we solve the sine-Gordon equation on the interval $\Omega =
diff --git a/deal.II/examples/step-26/doc/results.dox b/deal.II/examples/step-26/doc/results.dox
index e67fccc1c1..f4c6feefb5 100644
--- a/deal.II/examples/step-26/doc/results.dox
+++ b/deal.II/examples/step-26/doc/results.dox
@@ -1,2 +1 @@
-
In this section, we discuss a few results produced from running the
diff --git a/deal.II/examples/step-28/doc/results.dox b/deal.II/examples/step-28/doc/results.dox
index f7a468d988..5432205eb2 100644
--- a/deal.II/examples/step-28/doc/results.dox
+++ b/deal.II/examples/step-28/doc/results.dox
@@ -1,4 +1,4 @@
-
Results
+
Results
The output of this program consist of the console output, a file
diff --git a/deal.II/examples/step-3/doc/results.dox b/deal.II/examples/step-3/doc/results.dox
index 1ee4829f54..69018f874b 100644
--- a/deal.II/examples/step-3/doc/results.dox
+++ b/deal.II/examples/step-3/doc/results.dox
@@ -1,4 +1,3 @@
-
Results
The output of the program looks as follows:
diff --git a/deal.II/examples/step-4/doc/results.dox b/deal.II/examples/step-4/doc/results.dox
index cfd3be1c1f..0fa62e3ab7 100644
--- a/deal.II/examples/step-4/doc/results.dox
+++ b/deal.II/examples/step-4/doc/results.dox
@@ -1,4 +1,3 @@
-