Commit 47e36dc3 authored by Olivier's avatar Olivier

Chapter 3: swap two thumbnail videos (incorrect order)

parent 2b9c05d4
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\renewcommand{\numberofthischapter}{3}
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\end{IEEEeqnarray}
\end{mdframed}
\youtubethumb{VR8LGr6PuRY}{Making sense of the 3D linear momentum balance equation}{\oc (\ccby)}
\youtubethumb{iDCpqoJJSI4}{Making sense of the 3D linear momentum balance equation}{\oc (\ccby)}
Sometimes, the control volume has well-defined inlets and outlets through which the flow $\rho \vec V (\vec V_\rel \cdot \vec n)$ is uniform: this is illustrated again in figure~\ref{fig_cv_linearmom_simple}. In that case equation~\ref{eq_rtt_linearmom} reduces to forms that we have already identified in the previous chapter (see \S\ref{ch_balance_momentum_simple} p.~\pageref{ch_balance_momentum_simple}):
\begin{IEEEeqnarray}{rCl}
......@@ -248,7 +248,7 @@
\end{mdframed}
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\youtubethumb{iDCpqoJJSI4}{Making sense of the angular momentum balance equation}{\oc (\ccby)}
\youtubethumb{VR8LGr6PuRY}{Making sense of the angular momentum balance equation}{\oc (\ccby)}
Sometimes, the control volume has well-defined inlets and outlets through which the flow $\vec r_{\X m} \wedge \rho \vec V (\vec V_\rel \cdot \vec n)$ is uniform: this is illustrated in figure~\ref{fig_cv_angularmomentum_simple}. In that case equation~\ref{eq_rtt_angularmom} reduces to a more readable form:
\begin{IEEEeqnarray}{rCCCCCl}
\vec M_{\net, \X} & = & \timederivative{} \iiint_\cv \vec r_{\X m} \wedge \rho \vec V \diff \vol &+& \sum_\out \left\{ \vec r_{\X m} \wedge |\dot m| \vec V\right\} - \sum_\inn \left\{ \vec r_{\X m} \wedge |\dot m| \vec V\right\} \nonumber\\\label{eq_rtt_angularmom_simple}
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