2) Calculate the power radiated and the total power radiated P = Jd using Eq. (11.72) for the case where the velocity and acceleration of the particle are perpendicular. Example 11.3 does the same problem but for collinear v and a. Check that P is consistent with the Liénard formula Eq. (11.75). The solution of this problem can be used for circular motion, which is important for calculating synchrotron radiation. (See Problem 11.16.)
dP dΩ = 2.u Мос rad r² = q² i x (u xa)|2 (1 . u)5 16П2€о (11.72)
P= Moq²a²r6 бл с (11.75)
2) Calculate the power radiated and the total power radiated P = Jd using Eq. (11.72) for the case where the velocity an
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2) Calculate the power radiated and the total power radiated P = Jd using Eq. (11.72) for the case where the velocity an
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