this is for holding javascript data
Chris Spencer edited Theory.tex
about 10 years ago
Commit id: d4b4249c0cc9978177037c5068f563a5d21ed5b5
deletions | additions
diff --git a/Theory.tex b/Theory.tex
index 5781f2e..31ba66b 100644
--- a/Theory.tex
+++ b/Theory.tex
...
\section{Theory}
\center{Appleton's equation is given by}\[\eta^2=1-\frac{\omega_{pe}^2}{\omega^2\left((1+\frac{i\nu}{\omega})-\frac{\omega_{ce}^2\sin^2\theta}{2\omega^2\left(1-\frac{\omega_{pe}^2}{\omega^2}\right)}\pm\sqrt{\frac{(\omega_{ce}^2\sin^2\theta)^2}{4(1-\frac{\omega_{pe}^2}{\omega^2})}+\frac{\omega_{ce}^2cos^2\theta}{\omega^2}}\right)}\]for an infinite plasma[2]. This describes the index of refraction for a whistler wave where $\eta^2=\left(\frac{kc}{\omega}\right)^2$. $\omega_{pe}$ is the plasma frequency,$\omega_{ce}$ is the electron cyclotron frequency, and $\nu$ is the rate of collisions in the plasma.The angle $\theta$ refers to the angle the waves make with respect to the background magnetic field $B_0$.The first assumption made is that the first experiment's waves are made with $\theta=0$ for waves parallel to $B_0$ and that damping is slight so that $\nu\approx0$.Making these assumptions it is found that Appleton's equation reduces to
\[\n^2=1-\frac{\omega_{pe}^2}{(\omega+\omega_{ce})(\omega-\omega_{ce})\}. \[\n^2=1-\frac{\omega_{pe}^2}{(\omega+\omega_{ce})(\omega-\omega_{ce})\].