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Matteo Cantiello edited Mixed Modes.tex
about 9 years ago
Commit id: 312b684699719e6cacf886626352887b94888a24
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The radial displacement
\begin{equation}
\label{eqn:dr}
k_r^2=\bigg( k_r^2=\Bigg( 1 -
\frac{N^2}{\omega^2}\bigg) \bigg(1 \frac{N^2}{\omega^2}\Bigg) \Bigg(1 -
\frac{S_\ell^2}{\omega^2}\bigg)\,\frac{\omega^2}{c_s^2} \frac{S_\ell^2}{\omega^2}\Bigg)\,\frac{\omega^2}{c_s^2}
\end{equation}
Here, $\omega$ is the angular frequency of the wave, $N$ is the Brunt-Vaisala frequency, $S_\ell$ is the Lamb frequency for waves with harmonic degree $\ell$ and $c_s$ is the sound speed.