Classical Electrodynamics |
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Page 245
There will be a spectrum of eigenvalues y,” and corresponding solutions w, A = 1,
2, 3,..., which form an orthogonal set. These different solutions are called the
modes of the guide. For a given frequency o, the wave number k is determined
for ...
There will be a spectrum of eigenvalues y,” and corresponding solutions w, A = 1,
2, 3,..., which form an orthogonal set. These different solutions are called the
modes of the guide. For a given frequency o, the wave number k is determined
for ...
Page 310
When the frequency of the applied fields is comparable to v, the electrons have
time to accelerate and decelerate between collisions. Then inertial effects enter
and the conductivity becomes complex. Unfortunately at these same frequencies
...
When the frequency of the applied fields is comparable to v, the electrons have
time to accelerate and decelerate between collisions. Then inertial effects enter
and the conductivity becomes complex. Unfortunately at these same frequencies
...
Page
Consequently its spectrum will contain only a narrow range of frequencies
centered around yulb. In collision problems we must sum the frequency spectra (
15.52) over the various possible impact parameters. This gives the energy per
unit ...
Consequently its spectrum will contain only a narrow range of frequencies
centered around yulb. In collision problems we must sum the frequency spectra (
15.52) over the various possible impact parameters. This gives the energy per
unit ...
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 other sections not shown
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Common terms and phrases
acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 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 result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |