Classical Electrodynamics |
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Page 213
This means that at times immediately before t = 0 the wave consisted of two
pulses, both moving towards the origin, such that at t = 0 they coalesced into the
shape given by (7.38). Clearly at later times we expect each pulse to re-emerge
on ...
This means that at times immediately before t = 0 the wave consisted of two
pulses, both moving towards the origin, such that at t = 0 they coalesced into the
shape given by (7.38). Clearly at later times we expect each pulse to re-emerge
on ...
Page 436
Consequently AE = es V - E dt (13.22) where v = x, and in the dipole
approximation E is the field of the incident particle at the origin O. Using the
Fourier representations (13.16) and (13.17), as well as that for a delta function (
2.52), and the ...
Consequently AE = es V - E dt (13.22) where v = x, and in the dipole
approximation E is the field of the incident particle at the origin O. Using the
Fourier representations (13.16) and (13.17), as well as that for a delta function (
2.52), and the ...
Page 482
... loss of generality to lie in the z-z plane, making an angle 6 (the colatitude) with
the r axis. Only for very small 0 will there be appreciable radiation intensity. The
origin of time is chosen so that at t = 0 the particle is at the origin of coordinates.
... loss of generality to lie in the z-z plane, making an angle 6 (the colatitude) with
the r axis. Only for very small 0 will there be appreciable radiation intensity. The
origin of time is chosen so that at t = 0 the particle is at the origin of coordinates.
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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