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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 Oplasma ( 7.90 ) inserted for 0 : * k ? ~ ( 1 0p w2 ( 7.91 ) where 471ne = ( 7.92 ) т = 2 is called the ...
The propagation of transverse electromagnetic waves in a tenuous plasma is governed by equation ( 7.76 ) of Section 7.7 , with Oplasma ( 7.90 ) inserted for 0 : * k ? ~ ( 1 0p w2 ( 7.91 ) where 471ne = ( 7.92 ) т = 2 is called the ...
Page 322
10.4 Variation of azimuthal magnetic induction and pressure with radius in a cylindrical plasma column with a uniform current density J. 0 R The other model has the current density confined to a very thin layer on the surface , as is ...
10.4 Variation of azimuthal magnetic induction and pressure with radius in a cylindrical plasma column with a uniform current density J. 0 R The other model has the current density confined to a very thin layer on the surface , as is ...
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 .
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 .
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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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