## Classical Electrodynamics |

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Page 51

PROBLEMS 2.1 2.2 2.3 2.4 A point charge q is brought to a position a distance

daway from an infinite

of images, find: (a) the surface-charge density induced on the

PROBLEMS 2.1 2.2 2.3 2.4 A point charge q is brought to a position a distance

daway from an infinite

**plane**conductor held at zero potential. Using the methodof images, find: (a) the surface-charge density induced on the

**plane**, and plot it; ...Page 202

John David Jackson, Patrick Thaddeus Jackson.

This chapter is concerned with

infinite, media. The basic properties of

their ...

John David Jackson, Patrick Thaddeus Jackson.

**Plane**Electromagnetic WavesThis chapter is concerned with

**plane**waves in unbounded, or perhaps semi-infinite, media. The basic properties of

**plane**waves in nonconducting media—their ...

Page 220

E PARALLEL TO

2r + * sin 2i o" (i + r.) cos (i – r) Al * -- 2: ... (7.60) Eo" , sin 2i — sin 2r tan (i – r) - -

—o- - Eo sin 2r + 4. sin 2i tan (i + r.) Al Again the results on the right apply for u' ...

E PARALLEL TO

**PLANE**OF INCIDENCE Éd 2 us sin 2i —- 2 cos i sin r Eo ** sin2r + * sin 2i o" (i + r.) cos (i – r) Al * -- 2: ... (7.60) Eo" , sin 2i — sin 2r tan (i – r) - -

—o- - Eo sin 2r + 4. sin 2i tan (i + r.) Al Again the results on the right apply for u' ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

### Common terms and phrases

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