Classical Electrodynamics |
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Page 301
rapidly and cause the integrands to have very small average values except in the
forward direction where k < ko. In that direction the second term in both Fon and
Fm is unimportant, since the scattered field (9.117) is proportional to k x F. The ...
rapidly and cause the integrands to have very small average values except in the
forward direction where k < ko. In that direction the second term in both Fon and
Fm is unimportant, since the scattered field (9.117) is proportional to k x F. The ...
Page 473
14.4 Radiation pattern for charge accelerated in its direction of motion. The two
patterns are not to scale, the relativistic one (appropriate for y - 2) having been
reduced by a factor ~10° for the same acceleration. 6max therefore define the ...
14.4 Radiation pattern for charge accelerated in its direction of motion. The two
patterns are not to scale, the relativistic one (appropriate for y - 2) having been
reduced by a factor ~10° for the same acceleration. 6max therefore define the ...
Page 474
confined to a very narrow cone in the direction of motion. For such small angles
the angular distribution (14.39) can be written approximately dP(t') - 8 e^*.s (ys): -
14.41 10 oz., " (Toy (14.41) The natural angular unit is evidently y—".
confined to a very narrow cone in the direction of motion. For such small angles
the angular distribution (14.39) can be written approximately dP(t') - 8 e^*.s (ys): -
14.41 10 oz., " (Toy (14.41) The natural angular unit is evidently y—".
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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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