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But this component A, cannot be calculated by merely substituting J, into (5.32).
Equation (5.32) holds only for rectangular components of A.” Thus we write
rectangular components of J: J. = -J., sin o (5.34) J, = J., cos $' Since the
geometry is ...
But we have just seen that for comparable parallel and perpendicular forces the
radiation from the parallel component is negligible (of order 1/y”) compared to
that from the perpendicular component. Consequently we may neglect the
This has the obvious quantum interpretation that the radiation from a multipole of
order (l, m) carries off mh units of z component of angular momentum per photon
of energy hoo. In further analogy with quantum mechanics we would expect the ...
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Introduction to Electrostatics
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