aboutsummaryrefslogtreecommitdiff
path: root/content.tex
diff options
context:
space:
mode:
authorAdrian Kummerlaender2019-01-29 15:23:53 +0100
committerAdrian Kummerlaender2019-01-29 15:23:53 +0100
commitfe86c7399d9bc20f7f95f7557d6d2b80e7b86be3 (patch)
tree773832257283dd2c170e6d9ea01dc5d0e045fc6b /content.tex
parent75e67a53f648c0f7be39589723b5af7eecb666f1 (diff)
downloadgrid_refinement_bsc_thesis-fe86c7399d9bc20f7f95f7557d6d2b80e7b86be3.tar
grid_refinement_bsc_thesis-fe86c7399d9bc20f7f95f7557d6d2b80e7b86be3.tar.gz
grid_refinement_bsc_thesis-fe86c7399d9bc20f7f95f7557d6d2b80e7b86be3.tar.bz2
grid_refinement_bsc_thesis-fe86c7399d9bc20f7f95f7557d6d2b80e7b86be3.tar.lz
grid_refinement_bsc_thesis-fe86c7399d9bc20f7f95f7557d6d2b80e7b86be3.tar.xz
grid_refinement_bsc_thesis-fe86c7399d9bc20f7f95f7557d6d2b80e7b86be3.tar.zst
grid_refinement_bsc_thesis-fe86c7399d9bc20f7f95f7557d6d2b80e7b86be3.zip
Revamp gnuplot plotting to generate better output
Using the pdfcairo terminal for generating fluid flow plots in gnuplot using raw paraview-generated CSV exports generates high quality results. Sadly the resulting files are both unoptimized and quite big which leads to both large and unperformant documents (i.e. some PDF readers even crash) As an alternative this new gnuplot structure generates the fluid plot itself using the pngcairo terminal and includes the resulting high-resolution PNG image into a normal pdfcairo plot. This works out quite well. As a side benefit the plot scripts are now much easier to maintain.
Diffstat (limited to 'content.tex')
-rw-r--r--content.tex10
1 files changed, 5 insertions, 5 deletions
diff --git a/content.tex b/content.tex
index 241be7e..80127dd 100644
--- a/content.tex
+++ b/content.tex
@@ -938,7 +938,7 @@ Für die Umsetzung in OpenLB parametrisieren wir die Geometrie bezogen auf den Z
\begin{figure}[h]
\begin{adjustbox}{center}
-\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_unrefined_60s_full.pdf}
+\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_unrefined_60s.pdf}
\end{adjustbox}
\caption{Uniform mit \(N=20\) aufgelöstes Strömungsbild zu \(t=60s\)}
\label{fig:UniformCylinderVelocity60s}
@@ -948,7 +948,7 @@ Als Grundlage für den subjektiven Vergleich des Strömungsbildes simulieren wir
\begin{figure}[h]
\begin{adjustbox}{center}
-\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_single_refinement_60s_full.pdf}
+\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_single_refinement_60s.pdf}
\end{adjustbox}
\caption{Einfach verfeinertes Strömungsbild zu \(t=60s\)}
\label{fig:SingleLevelRefinementCylinderVelocity60s}
@@ -963,7 +963,7 @@ An dieser Stelle wollen wir die Gelegenheit nutzen, uns näher mit der Wahl der
\begin{figure}[h]
\begin{adjustbox}{center}
-\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_unrefined_60s_knudsen_full.pdf}
+\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_unrefined_60s_knudsen.pdf}
\end{adjustbox}
\caption{Verfeinerungskriterium in einem uniform aufgelösten Gitter zu \(t=60s\)}
\label{fig:UnrefinedCylinderKnudsen60s}
@@ -974,7 +974,7 @@ Große Teile des Gitters weisen demnach eine gute Auflösung mit Verfeinerungsfa
\begin{figure}[h]
\begin{adjustbox}{center}
-\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_single_refinement_60s_knudsen_full.pdf}
+\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_single_refinement_60s_knudsen.pdf}
\end{adjustbox}
\caption{Verfeinerungskriterium in einem einfach verfeinerten Gitter zu \(t=60s\)}
\label{fig:SingleLevelRefinementCylinderKnudsen60s}
@@ -984,7 +984,7 @@ Insgesamt war unter dieser formaleren Analyse unsere intuitive Wahl des in Abbil
\begin{figure}[h]
\begin{adjustbox}{center}
-\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_improved_grid_60s_knudsen_full.pdf}
+\includegraphics[width=1.2\textwidth]{img/static/cylinder2d_improved_grid_60s_knudsen.pdf}
\end{adjustbox}
\end{figure}