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 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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