## Classical Electrodynamics |

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Page 227

The propagation of transverse electromagnetic waves in a tenuous

governed by equation (7.76) of Section 7.7, with aplasma (7.90) inserted for or:* 2

2 k” - o s - #) (7.91) where 2 o, -o (7.92) m is called the

The propagation of transverse electromagnetic waves in a tenuous

**plasma**isgoverned by equation (7.76) of Section 7.7, with aplasma (7.90) inserted for or:* 2

2 k” - o s - #) (7.91) where 2 o, -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

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. Detailedanalysis” ...

Page 450

13.5 Energy Loss in an Electronic

particle passing through a

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 nonrelativisticparticle passing through a

**plasma**can be treated in a manner similar to thedensity effect for a relativistic particle. As was discussed in Section 10.10, the

length ...

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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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