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 | |
6 other sections not shown
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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 |