## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

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Page 2

1.2

useful to introduce a concept one step removed from the forces , the concept of

an

...

1.2

**Electric Field**Although the thing that eventually gets measured is a force , it isuseful to introduce a concept one step removed from the forces , the concept of

an

**electric field**due to some array of charged bodies . At the moment , the electric...

Page 9

If the path is closed , the line integral is zero , Edl = 0 ( 1.21 ) $ e . a result that can

also be obtained directly from Coulomb's ... 1.6 Surface Distributions of Charges

and Dipoles and Discontinuities in the

If the path is closed , the line integral is zero , Edl = 0 ( 1.21 ) $ e . a result that can

also be obtained directly from Coulomb's ... 1.6 Surface Distributions of Charges

and Dipoles and Discontinuities in the

**Electric Field**and Potential One of the ...Page 298

But far away from the hole ( in terms of its dimensions ) , although still “ near the

conducting plane , " the fields will be the same as if the hole were not there ,

namely , normal E , and tangential B. The

shown in ...

But far away from the hole ( in terms of its dimensions ) , although still “ near the

conducting plane , " the fields will be the same as if the hole were not there ,

namely , normal E , and tangential B. The

**electric field**lines might appear asshown in ...

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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