Classical Electrodynamics · Problem 14.9

Radiating Systems, Multipole Fields and Radiation — John David Jackson

Physics — E&M · synchrotron-radiation-energy-loss

Problem

A particle of mass mm, charge qq, moves in a plane perpendicular to a uniform, static, magnetic induction BB. (a) Calculate the total energy radiated per unit time, expressing it in terms of the constants already defined and the ratio γ\gamma of the particle's total energy to its rest energy. (b) If at time t=0t = 0 the particle has a total energy E0=γ0mc2E_0 = \gamma_0 mc^2, show that it will have energy E=γmc2<E0E = \gamma mc^2 < E_0 at a time tt, where t≈3m3c52q4B2(1γ−1γ0)t \approx \frac{3m^3 c^5}{2q^4 B^2}\left(\frac{1}{\gamma} - \frac{1}{\gamma_0}\right) provided γ≫1\gamma \gg 1. (c) If the particle is initially nonrelativistic and has a kinetic energy T0T_0 at t=0t = 0, what is its kinetic energy at time tt? (d) If the particle is actually trapped in the magnetic dipole field of the earth and is spiraling back and forth along a line of force, does it radiate more energy while near the equator, or while near its turning points? Why? Make quantitative statements if you can.

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