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@@ -820,14 +820,14 @@ Ideally, the ratio $\mathcal{C}_\mathcal{G}/\mathcal{C}_\mathcal{F}$ is small an
 \begin{figure}[!htb]
     \begin{center}
     \setlength\figureheight{0.35\textwidth}
-    \setlength\figurewidth{0.37\textwidth}
+    \setlength\figurewidth{0.35\textwidth}
     \subfigure[Performance scaling]{
 %        {\small\input{Chapters/chapter7/figures/PararealScaletestGTX590.tikz}}
-      \includegraphics[width=0.5\textwidth]{Chapters/chapter7/figures/PararealScaletestGTX590_conv.pdf}
+      \includegraphics[width=0.47\textwidth]{Chapters/chapter7/figures/PararealScaletestGTX590_conv.pdf}
     }
     \subfigure[Speedup]{
        % {\small\input{Chapters/chapter7/figures/PararealSpeedupGTX590.tikz}}
- \includegraphics[width=0.5\textwidth]{Chapters/chapter7/figures/PararealSpeedupGTX590_conv.pdf}
+ \includegraphics[width=0.47\textwidth]{Chapters/chapter7/figures/PararealSpeedupGTX590_conv.pdf}
     }
     \end{center}
     \caption[Parareal absolute timings and parareal speedup.]{(a) Parareal absolute timings for an increasingly number of water waves traveling one wave length, each wave resolution is ($33\times 9$). (b) Parareal speedup for two to sixteen compute nodes compared to the purely sequential single GPU solver. Notice how insensitive the parareal scheme is to the size of the problem solved. Test environment 2.}\label{ch7:fig:DDPA_SPEEDUP}