## Classical ElectrodynamicsProblems after each chapter |

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Page 181

4-11 6.5 Gauge Transformations ;

transformation ( 6.34 ) and ( 6.35 ) is called a gauge transformation , and the

invariance of the fields under such transformations is called gauge invariance .

The relation ...

4-11 6.5 Gauge Transformations ;

**Lorentz**Gauge ; Coulomb Gauge Thetransformation ( 6.34 ) and ( 6.35 ) is called a gauge transformation , and the

invariance of the fields under such transformations is called gauge invariance .

The relation ...

Page 392

Since we have discussed the

force density in Section 11.11 , we can immediately deduce the behavior of a

charged particle's momentum under

particles with ...

Since we have discussed the

**Lorentz**transformation properties of the**Lorentz**force density in Section 11.11 , we can immediately deduce the behavior of a

charged particle's momentum under

**Lorentz**transformations . For neutralparticles with ...

Page 632

Lifetime , of multipole transitions , 558 Ives - Stilwell experiment , 364 of pi

mesons in motion , 359 Light cone , 370 Jacobian , in

Linear superposition , of electric fields , 3 coordinates , 376 of plane waves , 203 ,

208 in ...

Lifetime , of multipole transitions , 558 Ives - Stilwell experiment , 364 of pi

mesons in motion , 359 Light cone , 370 Jacobian , in

**Lorentz**transformation ofLinear superposition , of electric fields , 3 coordinates , 376 of plane waves , 203 ,

208 in ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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