Classical Electrodynamics |
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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 477
14.7 Radiating particle illuminates the detector at O only for a time At. The
frequency spectrum thus contains frequencies up to a maximum or - (At)T". for
arbitrary motion it plays the role of a fundamental frequency of motion. Equation (
14.50) ...
14.7 Radiating particle illuminates the detector at O only for a time At. The
frequency spectrum thus contains frequencies up to a maximum or - (At)T". for
arbitrary motion it plays the role of a fundamental frequency of motion. Equation (
14.50) ...
Page 485
Then we find (pe = sys;) - slo); (14.85) p mc”/ p This critical frequency is seen to
agree with our qualitative estimate (14.50) of Section 14.4. If the motion of the
charge is truly circular, then clp is the fundamental frequency of rotation, wo.
Then we find (pe = sys;) - slo); (14.85) p mc”/ p This critical frequency is seen to
agree with our qualitative estimate (14.50) of Section 14.4. If the motion of the
charge is truly circular, then clp is the fundamental frequency of rotation, wo.
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
6 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 charged particle 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 shown in Fig shows side 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 |