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Find the radiation power developed by a non-relativistic particle with charge `e` and mass `m`, moving along a circular orbit of radius `R` in the field of a stationary point charge `q`.

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`dotoversetrarr(p) =(e)/(m) xx force = (e^(2)q)/(mR^(2)) (1)/(4piepsilon_(0))`.
Thus `P = (1)/((4piepsilon_(0))^(3)) ((e^(2)q)/(mR^(2)))^(2)(2)/(3c^(2))`.

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