## Classical Electrodynamics |

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Page 16

We want to show the uniqueness of the solution of Poisson's equation, V*q = —

47p,

conditions on the closed bounding surface S. We suppose, to the contrary, that

there exist ...

We want to show the uniqueness of the solution of Poisson's equation, V*q = —

47p,

**inside**a volume V subject to either Dirichlet or Neumann boundaryconditions on the closed bounding surface S. We suppose, to the contrary, that

there exist ...

Page 236

Then, just as in the static case, there is no electric field

charges

instantly in response to changes in the fields, no matter how rapid, and always ...

Then, just as in the static case, there is no electric field

**inside**the conductors. Thecharges

**inside**a perfect conductor are assumed to be so mobile that they moveinstantly in response to changes in the fields, no matter how rapid, and always ...

Page 259

8.8 Dielectric Wave Guides In Sections 8.2–8.5 we considered wave guides

made of hollow metal cylinders with fields only

structures are possible. The parallel-wire transmission line is an example. The

general ...

8.8 Dielectric Wave Guides In Sections 8.2–8.5 we considered wave guides

made of hollow metal cylinders with fields only

**inside**the hollow. Other guidingstructures are possible. The parallel-wire transmission line is an example. The

general ...

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### Contents

Introduction to Electrostatics | 1 |

Nº 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

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### Common terms and phrases

angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 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 result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written