## Classical ElectrodynamicsProblems after each chapter |

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Page 13

1.7 ] Introduction to Electrostatics 13

combined into one partial differential

-4πρ ( 1.28 ) This

where ...

1.7 ] Introduction to Electrostatics 13

**Equations**( 1.13 ) and ( 1.16 ) can becombined into one partial differential

**equation**for the single function Ø ( x ) : V2Φ-4πρ ( 1.28 ) This

**equation**is called Poisson's**equation**. In regions of spacewhere ...

Page 337

( Ate + ng ) n = 0 m an independent

the last two

independent of magnetic field , we suspect that there exist solutions of a purely ...

( Ate + ng ) n = 0 m an independent

**equation**, but may be derived by combiningthe last two

**equations**in ( 10.91 ) . Since the force**equation**in ( 10.91 ) isindependent of magnetic field , we suspect that there exist solutions of a purely ...

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 so...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Wave Guides and Resonant Cavities | 235 |

Copyright | |

5 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 coefficients 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