Wave transformation
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@ -107,23 +107,23 @@ Nonetheless, the gap between the values is still fairly small and the extreme wa
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\begin{figure*}
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\centering
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\includegraphics{fig/maxw.pdf}
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\caption{Free surface obtained with the SWASH model in two configurations. \textit{Case 1}: With breakwater;
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\caption{Free surface elevation obtained with the SWASH model in two configurations. \textit{Case 1}: With breakwater;
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\textit{Case 2}: Without breakwater.}\label{fig:swash}
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\end{figure*}
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\subsection{Wave propagation}
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\subsection{Wave transformation}
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The results from the large scale SWASH model using raw buoy measurements as a boundary conditions will be used in order
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to feed the small scale Olaflow model. Wave transformation is studied from the buoy to the breakwater. Those results
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show that the amplitude of the identified wave gets lower as the wave propagates over the domain. Nevertheless, a long
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trough precedes the crest, with a zone reaching 400m long where the water level is below 1m is present in front of the
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wave crest.
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The free surface obtained with the SWASH model using raw buoy measurements as an elevation boundary condition is
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plotted in Figure~\ref{fig:swash_trans}. Those results display a strong transformation of the wave between the buoy and
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the breakwater. Not only the amplitude, but also the shape of the wave are strongly impacted by the propagation over
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the domain. While the amplitude of the wave is reduced as the wave propagates shorewards, the length of the trough and
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the crest increases, with a zone reaching 400m long in front of the wave where the water level is below 0m.
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\begin{figure*}
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\centering
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\includegraphics{fig/x.pdf}
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\caption{Wave propagation from the buoy to the breakwater. \textit{The qualitative position of the wave is
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highlighted.}}\label{fig:trans}
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\caption{Propagation of the wave supposed to be responsible for the block displacement; highlighted zone:
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qualitatively estimated position of the wave.}\label{fig:swash_trans}
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\end{figure*}
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\subsection{Hydrodynamic conditions on the breakwater}
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