Classical Electrodynamics |
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Page 515
This sets a lower limit on impact parameters equal to (15.17), even for relativistic
motion. With (15.11), (15.12), and these revised impact parameters, the radiation
cross section x'(o') in the system K' is 16 Łes: ) () (o: 2) '(a)') co- + -—| – || || – || |n ...
This sets a lower limit on impact parameters equal to (15.17), even for relativistic
motion. With (15.11), (15.12), and these revised impact parameters, the radiation
cross section x'(o') in the system K' is 16 Łes: ) () (o: 2) '(a)') co- + -—| – || || – || |n ...
Page 572
In discussing the scattered intensity it is convenient to use the concept of a
scattering cross section. This has already been defined in (14.101). The scattered
power per unit solid angle is dPse c “too – — Irbse!” 16.153 ji==|rb. (16.153) The
...
In discussing the scattered intensity it is convenient to use the concept of a
scattering cross section. This has already been defined in (14.101). The scattered
power per unit solid angle is dPse c “too – — Irbse!” 16.153 ji==|rb. (16.153) The
...
Page 606
We see that near the resonant frequency oo the absorption cross section has the
same Lorentz shape as the scattering cross section, but is larger by a factor T/T.
At high frequencies T, -- oor, so that the absorption cross section approaches the
...
We see that near the resonant frequency oo the absorption cross section has the
same Lorentz shape as the scattering cross section, but is larger by a factor T/T.
At high frequencies T, -- oor, so that the absorption cross section approaches the
...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
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 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 |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |