## Classical Electrodynamics |

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Page 130

( b )

dielectric at r = a . 4 . 7 The following data on the variation of dielectric constant

with pressure are ...

( b )

**Calculate**the surface - charge distribution on the inner sphere . ( c )**Calculate**the polarization - charge density induced on the surface of thedielectric at r = a . 4 . 7 The following data on the variation of dielectric constant

with pressure are ...

Page 307

( a )

through the opening , using the vector Kirchhoff formula ( 9 . 82 ) with the

assumption that the tangential electric field in the opening is the unperturbed

incident ...

( a )

**Calculate**the diffracted fields and the power per unit solid angle transmittedthrough the opening , using the vector Kirchhoff formula ( 9 . 82 ) with the

assumption that the tangential electric field in the opening is the unperturbed

incident ...

Page 576

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

differential equation satisfied by Ez , 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 Ez , in order to simplify your

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle 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 modes 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 shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written