]> https://gitweb.dealii.org/ - dealii-svn.git/commitdiff
Fix table set-up for graphics.
authorwolf <wolf@0785d39b-7218-0410-832d-ea1e28bc413d>
Fri, 11 Feb 2000 10:04:12 +0000 (10:04 +0000)
committerwolf <wolf@0785d39b-7218-0410-832d-ea1e28bc413d>
Fri, 11 Feb 2000 10:04:12 +0000 (10:04 +0000)
git-svn-id: https://svn.dealii.org/trunk@2385 0785d39b-7218-0410-832d-ea1e28bc413d

deal.II/doc/reports/deal.II-paper/node5.html

index fac51116cb448d83916236910818ea876a319acb..5c11af13c752c9a86e2a33ad9638f9dc54a32d83 100644 (file)
@@ -107,7 +107,7 @@ such as the Euler equations of inviscid, eventually transonic flow.
  ALT="\includegraphics[width=0.4\textwidth]
 {pictures/conservation/burgers1.eps}">
     
-    
+</td><td>    
 <!-- MATH: $\includegraphics[width=0.4\textwidth]
 {pictures/conservation/burgers2.eps}$ -->
 <IMG
@@ -116,7 +116,7 @@ such as the Euler equations of inviscid, eventually transonic flow.
  ALT="\includegraphics[width=0.4\textwidth]
 {pictures/conservation/burgers2.eps}">
     
-    
+    </td><td>    
 <!-- MATH: $\includegraphics[width=0.4\textwidth]
 {pictures/conservation/euler.eps}$ -->
 <IMG
@@ -194,7 +194,7 @@ indispensable.
  SRC="img40.gif"
  ALT="\includegraphics[width=0.34\textwidth]
 {pictures/parameter/continuous_est.eps}">
-    
+    </td><td>    
 <!-- MATH: $\includegraphics[width=0.34\textwidth]
 {pictures/parameter/continuous_exact.eps}$ -->
 <IMG
@@ -202,7 +202,7 @@ indispensable.
  SRC="img41.gif"
  ALT="\includegraphics[width=0.34\textwidth]
 {pictures/parameter/continuous_exact.eps}">
-    
+    </td><td>    
 <!-- MATH: $\includegraphics[width=0.34\textwidth]
 {pictures/parameter/continuous_state.eps}$ -->
 <IMG
@@ -210,7 +210,7 @@ indispensable.
  SRC="img42.gif"
  ALT="\includegraphics[width=0.34\textwidth]
 {pictures/parameter/continuous_state.eps}">
-
+</td></tr><tr><td>    
 <!-- MATH: $\includegraphics[width=0.34\textwidth]
 {pictures/parameter/discontinuous_est.eps}$ -->
 <IMG
@@ -218,7 +218,7 @@ indispensable.
  SRC="img43.gif"
  ALT="\includegraphics[width=0.34\textwidth]
 {pictures/parameter/discontinuous_est.eps}">
-    
+    </td><td>    
 <!-- MATH: $\includegraphics[width=0.34\textwidth]
 {pictures/parameter/discontinuous_exact.eps}$ -->
 <IMG
@@ -226,7 +226,7 @@ indispensable.
  SRC="img44.gif"
  ALT="\includegraphics[width=0.34\textwidth]
 {pictures/parameter/discontinuous_exact.eps}">
-    
+    </td><td>    
 <!-- MATH: $\includegraphics[width=0.34\textwidth]
 {pictures/parameter/discontinuous_state.eps}$ -->
 <IMG
@@ -325,7 +325,7 @@ rather coarse cells were used where the solution is smooth.
  SRC="img48.gif"
  ALT="\includegraphics[width=0.3\textwidth]
 {pictures/wave3d/grid.0000.eps}">
-    
+    </td><td>    
     
 <!-- MATH: $\includegraphics[width=0.3\textwidth]
 {pictures/wave3d/grid.0020.eps}$ -->
@@ -335,7 +335,7 @@ rather coarse cells were used where the solution is smooth.
  ALT="\includegraphics[width=0.3\textwidth]
 {pictures/wave3d/grid.0020.eps}">
     
-    
+    </td><td>    
 <!-- MATH: $\includegraphics[width=0.3\textwidth]
 {pictures/wave3d/grid.0040.eps}$ -->
 <IMG
@@ -344,7 +344,7 @@ rather coarse cells were used where the solution is smooth.
  ALT="\includegraphics[width=0.3\textwidth]
 {pictures/wave3d/grid.0040.eps}">
     
-    
+    </td><td>    
 <!-- MATH: $\includegraphics[width=0.3\textwidth]
 {pictures/wave3d/grid.0060.eps}$ -->
 <IMG

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