Classical Electrodynamics |
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Page 412
The motion described by (12.93) is a circular motion perpendicular to B and a
uniform translation parallel to B. The solution for the velocity is easily shown to be
v(t) = uses + ora(e) – ies)e “” (12.95) where ea is a unit vector parallel to the field,
...
The motion described by (12.93) is a circular motion perpendicular to B and a
uniform translation parallel to B. The solution for the velocity is easily shown to be
v(t) = uses + ora(e) – ies)e “” (12.95) where ea is a unit vector parallel to the field,
...
Page 476
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.
Page 575
The uniform charge density of Problem 16.2 is replaced by a uniform density of
intrinsic magnetization parallel to the z axis and having total magnetic moment M.
With the same approximations as above calculate the nonvanishing radiation ...
The uniform charge density of Problem 16.2 is replaced by a uniform density of
intrinsic magnetization parallel to the z axis and having total magnetic moment M.
With the same approximations as above calculate the nonvanishing radiation ...
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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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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge 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 shows side 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 |