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Page 546
l, m - (16.47) E = > | ar(l, m)V x f(kr)Kim + a M(l, nooxwhere the coefficients an (l,
m) and a y(l, m) specify the amounts of electric (l, m) multipole and magnetic (l, m)
multipole fields. The radial functions f(kr) and g(kr) are of form (16.43).
l, m - (16.47) E = > | ar(l, m)V x f(kr)Kim + a M(l, nooxwhere the coefficients an (l,
m) and a y(l, m) specify the amounts of electric (l, m) multipole and magnetic (l, m)
multipole fields. The radial functions f(kr) and g(kr) are of form (16.43).
Page 549
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 ho. In further analogy with quantum mechanics we would expect 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 ho. In further analogy with quantum mechanics we would expect the ...
Page 557
The moment Qun is seen to be the same in form as the electrostatic multipole
moment qun (4.3). The moment Qin' is an induced electric multipole moment due
to the magnetization. It is generally at least a factor kr smaller than the normal ...
The moment Qun is seen to be the same in form as the electrostatic multipole
moment qun (4.3). The moment Qin' is an induced electric multipole moment due
to the magnetization. It is generally at least a factor kr smaller than the normal ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
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