update: auto commit

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2026-04-09 16:14:27 -04:00
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commit ad28c073ec
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@@ -246,6 +246,12 @@
\pdvt{u^I} + \tensor{A}{^i^I_J} \pdv{u^J}{x^i} = S^I, \pdvt{u^I} + \tensor{A}{^i^I_J} \pdv{u^J}{x^i} = S^I,
\end{equation} \end{equation}
where both $A$ and $S$ can depend on $u^I$ but not their derivatives. For any unit covector $\xi_i$, the \emph{Principal symbol} matrix is defined as $P(\xi) := \tensor{A}{^i^I_J} \xi_i$. where both $A$ and $S$ can depend on $u^I$ but not their derivatives. For any unit covector $\xi_i$, the \emph{Principal symbol} matrix is defined as $P(\xi) := \tensor{A}{^i^I_J} \xi_i$.
The system is said to be:
\begin{itemize}
\item \emph{weekly hyperbolic} if for any $\xi_i$, $P(\xi)$ has only real eigenvalues.
\item \emph{strongly hyperbolic} if for any $\xi_i$, $P(\xi)$ has only real eigenvalues and a complete set of eigenvectors, i.e., it is diagonalizable.
\item \emph{symmetrically hyperbolic} if there exists a positive definite symmetrizer matrix $H_{IJ}$ such that $H_{IK} \tensor{A}{^i^K_J}$ is symmetric for each $i$.
\end{itemize}
\end{frame} \end{frame}
\begin{frame}{Existing first order formulations} \begin{frame}{Existing first order formulations}