## Classical ElectrodynamicsProblems after each chapter |

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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 Oplasma ( 7.90 ) inserted for 0

: * WD ka ( 1 ( 7.91 ) w ? where 411n , e wp ( 7.92 ) m 2 0 is called the

The propagation of transverse electromagnetic waves in a tenuous

**plasma**isgoverned by equation ( 7.76 ) of Section 7.7 , with Oplasma ( 7.90 ) inserted for 0

: * WD ka ( 1 ( 7.91 ) w ? where 411n , e wp ( 7.92 ) m 2 0 is called the

**plasma**...Page 322

10.4 Variation of azimuthal magnetic induction and pressure with radius in a

cylindrical

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 with a uniform current density J. 0 R The other modelhas the current density confined to a very thin layer on the surface , as is

appropriate ...

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 ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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