more big output files removed

git-svn-id: https://svn.dealii.org/trunk@27756 0785d39b-7218-0410-832d-ea1e28bc413d

diff --git a/deal.II/examples/step-21/doc/results.dox b/deal.II/examples/step-21/doc/results.dox
index ad0d87e96bc68d7f25999c47530712920faaa847..b8c7d7892c48ed05b2560945f9f21adf70c4a58b 100644 (file)
--- a/deal.II/examples/step-21/doc/results.dox
+++ b/deal.II/examples/step-21/doc/results.dox
@@ -52,7 +52,7 @@ With all this, here are a few movies that show how the saturation progresses
 over time. First, this is for the single crack model, as implemented in the
 <code>SingleCurvingCrack::KInverse</code> class:
 
-@image html step-21.centerline.gif
+<img src="http://www.dealii.org/images/steps/developer/step-21.centerline.gif" alt="">
 
 As can be seen, the water rich fluid snakes its way mostly along the
 high-permeability zone in the middle of the domain, whereas the rest of the
@@ -66,14 +66,14 @@ The second movie shows the saturation for the random medium model of class
 centers of high permeability and fluid hops from one of these zones to
 the next:
 
-@image html step-21.random2d.gif
+<img src="http://www.dealii.org/images/steps/developer/step-21.random2d.gif" alt="">
 
 
 Finally, here is the same situation in three space dimensions, on a mesh with
 <code>n_refinement_steps=5</code>, which produces a mesh of some 32,000 cells
 and 167,000 degrees of freedom:
 
-@image html step-21.random3d.gif
+<img src="http://www.dealii.org/images/steps/developer/step-21.random3d.gif" alt="">
 
 To repeat these computations, all you have to do is to change the line
 @code

diff --git a/deal.II/examples/step-21/doc/step-21.centerline.gif b/deal.II/examples/step-21/doc/step-21.centerline.gif
deleted file mode 100644 (file)
index d7bc81e..0000000
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diff --git a/deal.II/examples/step-21/doc/step-21.random2d.gif b/deal.II/examples/step-21/doc/step-21.random2d.gif
deleted file mode 100644 (file)
index c5d025e..0000000
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diff --git a/deal.II/examples/step-21/doc/step-21.random3d.gif b/deal.II/examples/step-21/doc/step-21.random3d.gif
deleted file mode 100644 (file)
index 94d8fb8..0000000
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diff --git a/deal.II/examples/step-22/doc/results.dox b/deal.II/examples/step-22/doc/results.dox
index 437c499c8398c2eff739eda7b511609deea82323..3524d69293fcc2d9c33e847ab17e483545485f69 100644 (file)
--- a/deal.II/examples/step-22/doc/results.dox
+++ b/deal.II/examples/step-22/doc/results.dox
@@ -80,31 +80,31 @@ corners, so there is need for refinement there as well:
 <TABLE WIDTH="60%" ALIGN="center">
   <tr>
     <td ALIGN="center">
-      @image html step-22.2d.mesh-0.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.2d.mesh-0.png" alt="">
     </td>
 
     <td ALIGN="center">
-      @image html step-22.2d.mesh-1.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.2d.mesh-1.png" alt="">
     </td>
   </tr>
 
   <tr>
     <td ALIGN="center">
-      @image html step-22.2d.mesh-2.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.2d.mesh-2.png" alt="">
     </td>
 
     <td ALIGN="center">
-      @image html step-22.2d.mesh-3.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.2d.mesh-3.png" alt="">
     </td>
   </tr>
 
   <tr>
     <td ALIGN="center">
-      @image html step-22.2d.mesh-4.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.2d.mesh-4.png" alt="">
     </td>
 
     <td ALIGN="center">
-      @image html step-22.2d.mesh-5.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.2d.mesh-5.png" alt="">
     </td>
   </tr>
 </table>
@@ -113,7 +113,7 @@ Finally, following is a plot of the flow field. It shows fluid
 transported along with the moving upper boundary and being replaced by
 material coming from below:
 
-@image html step-22.2d.solution.png
+<img src="http://www.dealii.org/images/steps/developer/step-22.2d.solution.png" alt="">
 
 This plot uses the capability of VTK-based visualization programs (in
 this case of VisIt) to show vector data; this is the result of us
@@ -191,31 +191,31 @@ look as follow:
 <TABLE WIDTH="60%" ALIGN="center">
   <tr>
     <td ALIGN="center">
-      @image html step-22.3d.mesh-0.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d.mesh-0.png" alt="">
     </td>
 
     <td ALIGN="center">
-      @image html step-22.3d.mesh-1.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d.mesh-1.png" alt="">
     </td>
   </tr>
 
   <tr>
     <td ALIGN="center">
-      @image html step-22.3d.mesh-2.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d.mesh-2.png" alt="">
     </td>
 
     <td ALIGN="center">
-      @image html step-22.3d.mesh-3.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d.mesh-3.png" alt="">
     </td>
   </tr>
 
   <tr>
     <td ALIGN="center">
-      @image html step-22.3d.mesh-4.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d.mesh-4.png" alt="">
     </td>
 
     <td ALIGN="center">
-      @image html step-22.3d.mesh-5.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d.mesh-5.png" alt="">
     </td>
   </tr>
 </table>
@@ -224,7 +224,7 @@ Again, they show essentially the location of singularities introduced
 by boundary conditions. The vector field computed makes for an
 interesting graph:
 
-@image html step-22.3d.solution.png
+<img src="http://www.dealii.org/images/steps/developer/step-22.3d.solution.png" alt="">
 
 The isocountours shown here as well are those of the pressure
 variable, showing the singularity at the point of discontinuous
@@ -247,7 +247,7 @@ appropriately sorted into their corresponding blocks of the matrix and
 vector), then we get the following image after the first adaptive
 refinement in two dimensions:
 
-@image html step-22.2d.sparsity-nor.png
+<img src="http://www.dealii.org/images/steps/developer/step-22.2d.sparsity-nor.png" alt="">
 
 In order to generate such a graph, you have to insert a piece of
 code like the following to the end of the setup step.
@@ -268,7 +268,7 @@ In this program, we have thus chosen a more advanced renumbering of
 components.  The renumbering with DoFRenumbering::Cuthill_McKee and grouping
 the components into velocity and pressure yields the following output:
 
-@image html step-22.2d.sparsity-ren.png
+<img src="http://www.dealii.org/images/steps/developer/step-22.2d.sparsity-ren.png" alt="">
 
 It is apparent that the situation has improved a lot. Most of the elements are
 now concentrated around the diagonal in the (0,0) block in the matrix. Similar
@@ -288,7 +288,7 @@ considerable amount of tentative fill-in elements. This illustrates why UMFPACK
 is not a good choice in 3D - a full decomposition needs many new entries that
  eventually won't fit into the physical memory (RAM):
 
-@image html step-22.3d.sparsity_uu-ren.png
+<img src="http://www.dealii.org/images/steps/developer/step-22.3d.sparsity_uu-ren.png" alt="">
 
 
 
@@ -798,11 +798,11 @@ then we get images where the the fault line is curved:
 <TABLE WIDTH="60%" ALIGN="center">
   <tr>
     <td ALIGN="center">
-      @image html step-22.3d-extension.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d-extension.png" alt="">
     </td>
 
     <td ALIGN="center">
-      @image html step-22.3d-grid-extension.png
+      <img src="http://www.dealii.org/images/steps/developer/step-22.3d-grid-extension.png" alt="">
     </td>
   </tr>
 </table>

diff --git a/deal.II/examples/step-22/doc/step-22.2d.mesh-0.png b/deal.II/examples/step-22/doc/step-22.2d.mesh-0.png
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diff --git a/deal.II/examples/step-22/doc/step-22.2d.mesh-2.png b/deal.II/examples/step-22/doc/step-22.2d.mesh-2.png
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diff --git a/deal.II/examples/step-22/doc/step-22.2d.solution.png b/deal.II/examples/step-22/doc/step-22.2d.solution.png
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diff --git a/deal.II/examples/step-22/doc/step-22.3d.solution.png b/deal.II/examples/step-22/doc/step-22.3d.solution.png
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diff --git a/deal.II/examples/step-22/doc/step-22.3d.sparsity_uu-ren.png b/deal.II/examples/step-22/doc/step-22.3d.sparsity_uu-ren.png
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diff --git a/deal.II/examples/step-22/doc/step-22.profile-3.original.png b/deal.II/examples/step-22/doc/step-22.profile-3.original.png
deleted file mode 100644 (file)
index 1bea1c4..0000000
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diff --git a/deal.II/examples/step-22/doc/step-22.profile-3.png b/deal.II/examples/step-22/doc/step-22.profile-3.png
deleted file mode 100644 (file)
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diff --git a/deal.II/examples/step-23/doc/results.dox b/deal.II/examples/step-23/doc/results.dox
index 0fda35af8cb491319f579657a5c117b72f263639..d24f2ea369ac02cfed4dc0fc1adb83039bf39c7f 100644 (file)
--- a/deal.II/examples/step-23/doc/results.dox
+++ b/deal.II/examples/step-23/doc/results.dox
@@ -65,7 +65,7 @@ In addition to the screen output, the program writes the solution of each time
 step to an output file. If we process them adequately and paste them into a
 movie, we get the following:
 
-@image html step-23.movie.gif "Animation of the solution of step-23."
+<img src="http://www.dealii.org/images/steps/developer/step-23.movie.gif" alt="Animation of the solution of step-23.">
 
 The movie shows the generated wave nice traveling through the domain and back,
 being reflected at the clamped boundary. Some numerical noise is trailing the

diff --git a/deal.II/examples/step-23/doc/step-23.movie.gif b/deal.II/examples/step-23/doc/step-23.movie.gif
deleted file mode 100644 (file)
index 0ed0afa..0000000
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