## Classical Electrodynamics |

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Page 13

Poisson's

scalar ...

**Equations**(1.13) and (1.16) can be combined into one partial differential**equation**for the single function p(x): V*q = —4mp (1.28) This**equation**is calledPoisson's

**equation**. In regions of space where there is no charge density, thescalar ...

Page 54

Spherical and cylindrical geometries are first considered, and solutions of

Laplace's

of the various ordinary differential

...

Spherical and cylindrical geometries are first considered, and solutions of

Laplace's

**equation**are represented by ... Only an outline is given of the solutionof the various ordinary differential

**equations**obtained from Laplace's**equation**by...

Page 582

The

rather than first, and therefore runs counter to the well-known requirements for a

dynamical

The

**equation**can be criticized on the grounds that it is second order in time,rather than first, and therefore runs counter to the well-known requirements for a

dynamical

**equation**of motion. This difficulty manifests itself immediately in the ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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### Common terms and phrases

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 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