Calculate the radiation damping of a charged particle attached to a spring of natural frequency ω_0, driven at frequency ω.
Calculate the radiation damping of a charged particle attached to a spring of natural frequency ω_0, driven at frequency ω.
The equation of motion is
m\ddot{x}=F_{spring}+F_{rad}+F{driving}=-m\omega ^{2}_{0}x+m\tau \overset{…}{x} +F_{driving}.With the system oscillating at frequency ω,
x(t)=x_{0}\cos(\omega t +\delta ),so
\overset{…}{x} =-\omega ^{2}\dot{x}.Therefore
m\ddot{x} + mγ\dot{x} + m\omega ^2_0x =F_{driving}, (11.83)
and the damping factor γ is given by
γ = ω^2τ. (11.84)
[When I wrote F_{damping} = −γmv, back in Chap. 9 (Eq. 9.152), I assumed for simplicity that the damping was proportional to the velocity. We now know that radiation damping, at least, is proportional to \ddot{v}. But it hardly matters: for sinusoidal oscillations any even number of derivatives of v would do, since they’re all proportional to v.]
F_{damping} = −mγ \frac{dx}{dt} . (9.152)