## 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 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written