Classical Electrodynamics |
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Page 269
The electromagnetic potentials and fields are assumed to have the same time
dependence. It was shown in Chapter 6 that the solution for the vector potential A
(x, t) in the Lorentz gauge is A(x, t) = Jersar J(x', t') •(r + B = <! — i) (9.2) c c |x — x"|
...
The electromagnetic potentials and fields are assumed to have the same time
dependence. It was shown in Chapter 6 that the solution for the vector potential A
(x, t) in the Lorentz gauge is A(x, t) = Jersar J(x', t') •(r + B = <! — i) (9.2) c c |x — x"|
...
Page 296
Both formulas contain the same “diffraction” distribution factor [J.(kaš)|kaśl and
the same dependence on wave number. But the scalar result has no azimuthal
dependence (apart from that contained in 5), whereas the vector expression does
.
Both formulas contain the same “diffraction” distribution factor [J.(kaš)|kaśl and
the same dependence on wave number. But the scalar result has no azimuthal
dependence (apart from that contained in 5), whereas the vector expression does
.
Page 553
Furthermore, we assume that the time dependence can be analyzed into its
Fourier components, and we consider only harmonically varying sources, - p(x)e^
*, J(x)e^*', M(x)e^* (16.76) where it is understood that we take the real part of
such ...
Furthermore, we assume that the time dependence can be analyzed into its
Fourier components, and we consider only harmonically varying sources, - p(x)e^
*, J(x)e^*', M(x)e^* (16.76) where it is understood that we take the real part of
such ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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