## Classical Electrodynamics |

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Page 25

1.5 cm 7 5.0 cm 2 (a) For the three capacitor geometries in Problem 1.5 calculate

the total

opposite charges Q and – Q placed on the conductors and the potential ...

1.5 cm 7 5.0 cm 2 (a) For the three capacitor geometries in Problem 1.5 calculate

the total

**electrostatic**energy and express it alternatively in terms of the equal andopposite charges Q and – Q placed on the conductors and the potential ...

Page 145

We note a characteristic difference between this problem and a corresponding

cylindrically symmetric

appear, as well as ordinary Legendre polynomials. This can be traced to the

vector ...

We note a characteristic difference between this problem and a corresponding

cylindrically symmetric

**electrostatic**problem. Associated Legendre polynomialsappear, as well as ordinary Legendre polynomials. This can be traced to the

vector ...

Page 634

... 463 Multipole,

101

magnetostatic, 145 radiating, near, induction, and radiation zones, 270 time-

varying ...

... 463 Multipole,

**electrostatic**, 98**electrostatic**, expansion of interaction energy in,101

**electrostatic**, expansion of potential in, 98**electrostatic**, rectangular, 100magnetostatic, 145 radiating, near, induction, and radiation zones, 270 time-

varying ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

5 other sections not shown

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