Classical Electrodynamics |
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Page 402
most. +*H*). +:[1-(*#")||1-(**)]"co,. q249. where E' is given by (12.31). To obtain E,
we merely interchange ms and m, and change 0' into T – 6' (cos 0' → —cos 0').
The relation between angles 6' and 62 can be obtained from the expression ...
most. +*H*). +:[1-(*#")||1-(**)]"co,. q249. where E' is given by (12.31). To obtain E,
we merely interchange ms and m, and change 0' into T – 6' (cos 0' → —cos 0').
The relation between angles 6' and 62 can be obtained from the expression ...
Page 446
The Fermi expression (13.70) bears little resemblance to our previous results for
energy loss, such as (13.35). But under conditions where polarization effects are
unimportant it yields the same results as before. For example, for nonrelativistic ...
The Fermi expression (13.70) bears little resemblance to our previous results for
energy loss, such as (13.35). But under conditions where polarization effects are
unimportant it yields the same results as before. For example, for nonrelativistic ...
Page 447
where we have used the dipole moment expression (13.19). Assuming that the
second term is small, the imaginary part of 1/e(a) can be readily calculated and
substituted into (13.70). Then the integral over do can be performed in the same ...
where we have used the dipole moment expression (13.19). Assuming that the
second term is small, the imaginary part of 1/e(a) can be readily calculated and
substituted into (13.70). Then the integral over do can be performed in the same ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
16 other sections not shown
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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 limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes 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 |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |