## Classical Electrodynamics |

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Page 25

1.7 1.8 1.9 1.10 1.11 Show that the capacitance per unit length is

approximately by –1 C ~ ... derivative of the electric field is

= - || - + - E on R1 R2 where R, and R, are the principal radii of curvature of the

surface.

1.7 1.8 1.9 1.10 1.11 Show that the capacitance per unit length is

**given**approximately by –1 C ~ ... derivative of the electric field is

**given**by 1 9E 1 1 — —= - || - + - E on R1 R2 where R, and R, are the principal radii of curvature of the

surface.

Page 229

For propagation in directions other than parallel to the static field Bo it is

straightforward to show that, if terms of the order of op” are neglected compared

to o” and oop, the index of refraction is still

frequency ...

For propagation in directions other than parallel to the static field Bo it is

straightforward to show that, if terms of the order of op” are neglected compared

to o” and oop, the index of refraction is still

**given**by (7.102). But the precessionfrequency ...

Page 305

More complete discussions of antennas and antenna arrays are

engineering works, such as Jordan, Kraus, Schelkunoff, Silver. The subject of

diffraction has a very extensive literature. A comprehensive treatment of both the

scalar ...

More complete discussions of antennas and antenna arrays are

**given**inengineering works, such as Jordan, Kraus, Schelkunoff, Silver. The subject of

diffraction has a very extensive literature. A comprehensive treatment of both the

scalar ...

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### Contents

Introduction to Electrostatics | 1 |

Nš 3 | 3 |

Greens theorem | 14 |

Copyright | |

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