Classical Electrodynamics |
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Page 236
8.1 Fields at the Surface of and within a Conductor As was mentioned at the end
of Section 7.7, the problem of reflection and refraction of waves at an interface of
two conducting media is somewhat complicated. The most important and useful ...
8.1 Fields at the Surface of and within a Conductor As was mentioned at the end
of Section 7.7, the problem of reflection and refraction of waves at an interface of
two conducting media is somewhat complicated. The most important and useful ...
Page 238
0; neglecting the other derivatives when operating on the fields within the
conductor. With this approximation (8.5) become: E. c. – –– n x * 4tro 65 (8.6) H, c
- + n x 0E. Auo 05 These can be combined to yield 22 2i ão" x Hot in x H,) - 0 (8.7)
and ...
0; neglecting the other derivatives when operating on the fields within the
conductor. With this approximation (8.5) become: E. c. – –– n x * 4tro 65 (8.6) H, c
- + n x 0E. Auo 05 These can be combined to yield 22 2i ão" x Hot in x H,) - 0 (8.7)
and ...
Page 240
*0. – i)(n x Ho)e^*** (8.13) 7. The time-average rate of dissipation of energy per
unit volume in ohmic losses is $J. E* = (1/20) |J|*, so that the total rate of energy
dissipation in the conductor for the volume lying beneath an area element AA is 1
.
*0. – i)(n x Ho)e^*** (8.13) 7. The time-average rate of dissipation of energy per
unit volume in ohmic losses is $J. E* = (1/20) |J|*, so that the total rate of energy
dissipation in the conductor for the volume lying beneath an area element AA is 1
.
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Contents
Introduction to Electrostatics | 1 |
Nº 3 | 3 |
Greens theorem | 14 |
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 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 |