Classical Electrodynamics |
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Page 220
E PARALLEL TO PLANE OF INCIDENCE * = 2 Le sin 2i —o- 2 cos i sin r Eo **
sin 2r + * sin 2i o" (i + r.) cos (i — r) pr * sin 2i — sin 2r - (7.60) Eo" — 4 -> tan (i —
r) * in 2, 14 in 2: "( t ) Au Again the results on the right apply for u' = u. For normal
...
E PARALLEL TO PLANE OF INCIDENCE * = 2 Le sin 2i —o- 2 cos i sin r Eo **
sin 2r + * sin 2i o" (i + r.) cos (i — r) pr * sin 2i — sin 2r - (7.60) Eo" — 4 -> tan (i —
r) * in 2, 14 in 2: "( t ) Au Again the results on the right apply for u' = u. For normal
...
Page
E is parallel to the r axis; B is parallel to the y axis. (a) For |E| < |B] make the
necessary Lorentz transformation described in Section 12.8 to obtain explicitly
parametric equations for the particle's trajectory. (b) Repeat the calculation of (a)
for |E| ...
E is parallel to the r axis; B is parallel to the y axis. (a) For |E| < |B] make the
necessary Lorentz transformation described in Section 12.8 to obtain explicitly
parametric equations for the particle's trajectory. (b) Repeat the calculation of (a)
for |E| ...
Page
parallel to and perpendicular to the velocity. But we have just seen that for
comparable parallel and perpendicular forces the radiation from the parallel
component is negligible (of order 1/y”) compared to that from the perpendicular
component.
parallel to and perpendicular to the velocity. But we have just seen that for
comparable parallel and perpendicular forces the radiation from the parallel
component is negligible (of order 1/y”) compared to that from the perpendicular
component.
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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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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 |
| Authors | John David Jackson, Patrick Thaddeus Jackson |
| Edition | 3 |
| Publisher | Wiley, 1962 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |