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reidmen 2022-04-11 18:23:05 +02:00
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cbme2022/CMBE21_ale.tex
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@ -109,7 +109,7 @@ We will show the extension to a CT scheme. Namely, in that case the following in
\end{equation} \end{equation}
for $(\mathbf{u}^n, p^n)$ the velocity/pressure pair solution at time $t^n$, in the reference domain $\Omega^0$, for operators to be specified in the talk. for $(\mathbf{u}^n, p^n)$ the velocity/pressure pair solution at time $t^n$, in the reference domain $\Omega^0$, for operators to be specified in the talk.
Our finding will be supplemented with an application to fluid-solid interaction in an idealized cardiac geometry, exploiting the splitting nature of the CT scheme with a well-known coupling approach \cite{bertoglio2013sisc}. \textcolor{red}{cita el paper original de fernandez, gerbau y grandmont porfa} Our finding will be supplemented with an application to fluid-solid interaction in an idealized cardiac geometry, exploiting the splitting nature of the CT scheme with a well-known coupling approach \cite{bertoglio2013sisc, fernandez-gerbeau-grandmont-06}.
%In such a case, we will exploit the fluid pressure projection step, coupling it with the solid problem in an efficient fashion. Simulations of such a case will be provided, as well as the current research done in more realistic geometries. %In such a case, we will exploit the fluid pressure projection step, coupling it with the solid problem in an efficient fashion. Simulations of such a case will be provided, as well as the current research done in more realistic geometries.
\begin{figure}[!hbtp] \begin{figure}[!hbtp]
\centering \centering
@ -118,7 +118,7 @@ Our finding will be supplemented with an application to fluid-solid interaction
\label{fig:comparison_figure} \label{fig:comparison_figure}
\end{figure} \end{figure}
%\newpage \newpage
\bibliography{biblio_merged.bib} \bibliography{biblio_merged.bib}