Classical Electrodynamics |
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Page 227
The propagation of transverse electromagnetic waves in a tenuous plasma is
governed by equation (7.76) of Section 7.7, with oblasma (7.90) inserted for or:* 2
2 k” - . ( - #) (7.91) where 2 o, - *** (7.92) m is called the plasma frequency.
The propagation of transverse electromagnetic waves in a tenuous plasma is
governed by equation (7.76) of Section 7.7, with oblasma (7.90) inserted for or:* 2
2 k” - . ( - #) (7.91) where 2 o, - *** (7.92) m is called the plasma frequency.
Page 329
It is clear qualitatively that it must be possible, by a combination of trapped axial
field and conducting walls, to create a stable configuration, at least in the
approximation of a highly conducting plasma with a sharp boundary. Detailed
analysis” ...
It is clear qualitatively that it must be possible, by a combination of trapped axial
field and conducting walls, to create a stable configuration, at least in the
approximation of a highly conducting plasma with a sharp boundary. Detailed
analysis” ...
Page 450
13.5 Energy Loss in an Electronic Plasma The loss of energy by a nonrelativistic
particle passing through a plasma can be treated in a manner similar to the
density effect for a relativistic particle. As was discussed in Section 10.10, the
length ...
13.5 Energy Loss in an Electronic Plasma The loss of energy by a nonrelativistic
particle passing through a plasma can be treated in a manner similar to the
density effect for a relativistic particle. As was discussed in Section 10.10, the
length ...
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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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