From 63530d552e04b556857cbd9796ce01b0c6822214 Mon Sep 17 00:00:00 2001 From: Timo Heister Date: Mon, 13 May 2019 12:08:00 -0600 Subject: [PATCH] use doxygen style for html tables with border --- examples/step-20/doc/results.dox | 4 ++-- examples/step-29/doc/results.dox | 4 ++-- examples/step-31/doc/results.dox | 10 +++++----- examples/step-32/doc/results.dox | 2 +- examples/step-37/doc/results.dox | 2 +- examples/step-48/doc/results.dox | 2 +- examples/step-51/doc/results.dox | 2 +- examples/step-59/doc/results.dox | 4 ++-- 8 files changed, 15 insertions(+), 15 deletions(-) diff --git a/examples/step-20/doc/results.dox b/examples/step-20/doc/results.dox index 8f43a30be9..abd88fce73 100644 --- a/examples/step-20/doc/results.dox +++ b/examples/step-20/doc/results.dox @@ -75,7 +75,7 @@ the program run. If one does this, one finds the following pattern for the $L_2$ error in the pressure variable: - +
@@ -119,7 +119,7 @@ experimentally observed ones indicated in the last row of the table. One can make the same experiment with the $L_2$ error in the velocity variables: -
Finite element order
+
diff --git a/examples/step-29/doc/results.dox b/examples/step-29/doc/results.dox index 3185cdad21..a7bf550135 100644 --- a/examples/step-29/doc/results.dox +++ b/examples/step-29/doc/results.dox @@ -81,7 +81,7 @@ DEAL::Generating output... done (0.720528s) The graphical output of the program looks as follows: -
Finite element order
+
v = Re(u) @@ -109,7 +109,7 @@ Because colorful graphics are always fun, and to stress the focusing effects some more, here is another set of images highlighting how well the intensity is actually focused in $x$-direction: - +
|u| diff --git a/examples/step-31/doc/results.dox b/examples/step-31/doc/results.dox index b92d010eaf..9bedcf5529 100644 --- a/examples/step-31/doc/results.dox +++ b/examples/step-31/doc/results.dox @@ -86,7 +86,7 @@ The program runs for a while. The temperature field for time steps 0, 500, 1000, 1500, 2000, 3000, 4000, and 5000 looks like this (note that the color scale used for the temperature is not always the same): - +
@@ -136,7 +136,7 @@ equation we have chosen. In addition to the pictures above, the following ones show the adaptive mesh and the flow field at the same time steps: - +
@@ -240,7 +240,7 @@ Visualizing the temperature isocontours at time steps 0, 50, 100, 150, 200, 300, 400, 500, 600, 700, and 800 yields the following plots: - +
@@ -408,7 +408,7 @@ Here is what we get for $\beta=0.01, \beta=0.1$, and $\beta=0.5$, different choices of $c_k$, and bilinear elements (temperature_degree=1) in 2d: - +
@@ -484,7 +484,7 @@ elements as well. Here are the graphs for bi-quadratic shape functions (temperature_degree=2) for the temperature, while we retain the $Q_2/Q_1$ stable Taylor-Hood element for the Stokes system: - +
diff --git a/examples/step-32/doc/results.dox b/examples/step-32/doc/results.dox index 6e62c9e8ce..39568baae4 100644 --- a/examples/step-32/doc/results.dox +++ b/examples/step-32/doc/results.dox @@ -19,7 +19,7 @@ meshes had around 72,000 and 236,000 cells, for a total of 2,680,000 and 8,250,000 degrees of freedom, respectively, more than an order of magnitude more than we had available in step-31: - +
diff --git a/examples/step-37/doc/results.dox b/examples/step-37/doc/results.dox index db5fb60b7b..2e933735c9 100644 --- a/examples/step-37/doc/results.dox +++ b/examples/step-37/doc/results.dox @@ -213,7 +213,7 @@ support, i.e., four operations on doubles can be done with one CPU instruction, which is heavily used in FEEvaluation), optimized mode, and two MPI ranks. - +
diff --git a/examples/step-48/doc/results.dox b/examples/step-48/doc/results.dox index bc4b029f3b..baad8d2948 100644 --- a/examples/step-48/doc/results.dox +++ b/examples/step-48/doc/results.dox @@ -11,7 +11,7 @@ wave equation (the sine-term skipped from the sine-Gordon equation). We use both second and fourth order elements. The results are summarized in the following table. -
  Sparse matrix
+
diff --git a/examples/step-51/doc/results.dox b/examples/step-51/doc/results.dox index 6d88fd76a1..284f3ac598 100644 --- a/examples/step-51/doc/results.dox +++ b/examples/step-51/doc/results.dox @@ -304,7 +304,7 @@ problems). Let us look at the computing time of the tutorial program and the share of the individual components: -
  wave equation
+
diff --git a/examples/step-59/doc/results.dox b/examples/step-59/doc/results.dox index 2c6f975c76..541e84055c 100644 --- a/examples/step-59/doc/results.dox +++ b/examples/step-59/doc/results.dox @@ -126,7 +126,7 @@ million degrees of freedom solved per second (MDoFs/s) to be able to compare the efficiency of the different degrees, which is computed by dividing the number of degrees of freedom by the solver time. -
   
+
@@ -237,7 +237,7 @@ basic FE_DGQ elements where both the MPI exchange are more expensive and the operations done by FEFaceEvaluation::gather_evaluate() and FEFaceEvaluation::integrate_scatter(). -
degree 1
+
-- 2.39.5
degree 1