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 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Authors | John David Jackson, Patrick Thaddeus Jackson |
| Edition | 3 |
| Publisher | Wiley, 1962 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |