Classical Electrodynamics |
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Page 248
2 (E x H*) (8.47) whose real part gives the time-averaged flux of energy. For the
two types of field we find, using (8.24): 2 ok lovo + i . ww. S = ±, (8.48) 8try" | 1 • ?".
=|es IV, pl" — i + p^V,"p Al k where the upper (lower) line is for TM (TE) modes.
2 (E x H*) (8.47) whose real part gives the time-averaged flux of energy. For the
two types of field we find, using (8.24): 2 ok lovo + i . ww. S = ±, (8.48) 8try" | 1 • ?".
=|es IV, pl" — i + p^V,"p Al k where the upper (lower) line is for TM (TE) modes.
Page 273
... one of which gives a transverse magnetic induction and the other of which
gives a transverse electric field. These physically distinct contributions can be
separated. [Sect. 9.3] Simple Radiating Systems and Diffraction 273 Magnetic
dipole ...
... one of which gives a transverse magnetic induction and the other of which
gives a transverse electric field. These physically distinct contributions can be
separated. [Sect. 9.3] Simple Radiating Systems and Diffraction 273 Magnetic
dipole ...
Page 366
This interaction energy gives the anomalous Zeeman effect correctly, but has a
spin-orbit interaction which is twice too large. The error in (11.45) can be traced
to the incorrectness of (11.40) as an equation of motion for the electron spin.
This interaction energy gives the anomalous Zeeman effect correctly, but has a
spin-orbit interaction which is twice too large. The error in (11.45) can be traced
to the incorrectness of (11.40) as an equation of motion for the electron spin.
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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 |