## Classical ElectrodynamicsProblems after each chapter |

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Page 181

6.5 Gauge Transformations ;

6.5 Gauge Transformations ;

**Lorentz**Gauge ; Coulomb Gauge The transformation ( 6.34 ) and ( 6.35 ) is called a gauge transformation , and the invariance of ...Page 367

At time t the electron's rest frame K'and the laboratory frame K are related by a

At time t the electron's rest frame K'and the laboratory frame K are related by a

**Lorentz**transformation with velocity v . At time 1 + dt the electron's ...Page

Ives - Stilwell experiment , 364 Jacobian , in

Ives - Stilwell experiment , 364 Jacobian , in

**Lorentz**transformation of coordinates , 376 in transforming delta functions , 79 Kinematics , relativistic ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

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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 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 sphere spherical surface transformation unit vanishes vector velocity volume wave written