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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 aplasma (7.90) inserted for or:* 2
2 k? ~ . ( - #) (7.91) where 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 aplasma (7.90) inserted for or:* 2
2 k? ~ . ( - #) (7.91) where o, - *** (7.92) m is called the plasma frequency.
Page 322
10.4 Variation of azimuthal magnetic induction and pressure with radius in a
cylindrical plasma column O R r with a uniform current density J. The other model
has the current density confined to a very thin layer on the surface, as is
appropriate ...
10.4 Variation of azimuthal magnetic induction and pressure with radius in a
cylindrical plasma column O R r with a uniform current density J. The other model
has the current density confined to a very thin layer on the surface, as is
appropriate ...
Page 323
A simple model, first discussed by M. Rosenbluth, exhibits the essential
dynamical features. Suppose that a plasma is created in a hollow conducting
cylinder of radius Ro and length L. A voltage difference V is applied between the
ends of the ...
A simple model, first discussed by M. Rosenbluth, exhibits the essential
dynamical features. Suppose that a plasma is created in a hollow conducting
cylinder of radius Ro and length L. A voltage difference V is applied between the
ends of the ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
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