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Radiation

< PlasmaWiki(Link to this page as [[PlasmaWiki/Radiation]])

The power radiated by an accelerated charge is given (for non-relativistic particles) by:

$\frac{dP}{d\Omega}=\frac{q^2 \dot{v}^2}{16 \pi^2 \epsilon_0 c^3}\sin^2 \theta$

Where $θ$ is the angle from the direction of acceleration. Integrating over the solid angle:

$P=\frac{\pi e^2 \dot{v}^2}{6 \pi^2 \epsilon_0 c^3}$

This page was recovered in October 2009 from the Plasmagicians page on Radiation dated 19:36, 18 April 2007.