## Classical Electrodynamics |

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Page 130

(b)

the polarization-charge density induced on the surface of the dielectric at r = a.

4.7 The following data on the variation of dielectric constant with pressure are

taken ...

(b)

**Calculate**the surface-charge distribution on the inner sphere. (c)**Calculate**the polarization-charge density induced on the surface of the dielectric at r = a.

4.7 The following data on the variation of dielectric constant with pressure are

taken ...

Page 575

Keeping only lowest-order terms in B and making the long-wavelength

approximation,

distribution of radiation, and the total power radiated. The uniform charge density

of Problem ...

Keeping only lowest-order terms in B and making the long-wavelength

approximation,

**calculate**the nonvanishing multipole moments, the angulardistribution of radiation, and the total power radiated. The uniform charge density

of Problem ...

Page 576

to the energy in the field. ... to perform some integrations by parts, and to use the

differential equation satisfied by E., in order to simplify your

**Calculate**the ratio of the z component of the electromagnetic angular momentumto the energy in the field. ... to perform some integrations by parts, and to use the

differential equation satisfied by E., in order to simplify your

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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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