diff --git a/report/chapters/olaflow.tex b/report/chapters/olaflow.tex
index 7d4b2dc..875a237 100644
--- a/report/chapters/olaflow.tex
+++ b/report/chapters/olaflow.tex
@@ -100,8 +100,16 @@ The value of $b$ seems to have a major effect how wave energy is dissipated / ho
 A case with the $k-\omega$ SST turbulence model was run to compare with the $k-\varepsilon$ model.
 Results displayed in \autoref{fig:sst}. Significant differences are found between both models.
 
+Wave breaking as expected using SST model (\autoref{fig:sst175}). See
+\url{https://public.edgarpierre.fr/anim_olaflow_kom.mp4}
+
 \begin{figure}
 	\centering
 	\includegraphics{diffsst.pdf}
-	\caption{Case 1: $k-\varepsilon$ model; case 2: $k-\omega$ SST model.}\label{fig:sst}
+	\caption{$x=\SI{-50}{\m}$. Case 1: $k-\varepsilon$ model; case 2: $k-\omega$ SST model.}\label{fig:sst}
+\end{figure}
+\begin{figure}
+	\centering
+	\includegraphics{diffsst175.pdf}
+	\caption{$t=\SI{175}{\s}$. Case 1: $k-\varepsilon$ model; case 2: $k-\omega$ SST model.}\label{fig:sst175}
 \end{figure}
diff --git a/report/fig/diffsst175.pdf b/report/fig/diffsst175.pdf
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