lanebeale edited Theory.tex  about 10 years ago

Commit id: d594b9c3812e8cc34e58a6020c13d6204389a0ca

deletions | additions      

       

\end{tiny}  One of the remarkable aspects of ducted whistler waves is that the phase velocity travels at a separate angle to the group velocity and direction of propogation of the wave. The group velocity is given by  $\vec{V}_{gr}=\frac{\mathrm\partial\omega}{\mathrm \partial\vec{k}} \partial\vec{k}}$