## Classical Electrodynamics |

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Page 181

5 Gauge Transformations ;

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 ( 6 .

5 Gauge Transformations ;

**Lorentz**Gauge ; Coulomb Gauge The 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 ( 6 .

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 ...

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 ...

Page 632

Ives-Stilwell experiment, 364 Jacobian, in

376 in transforming delta functions, 79 Kinematics, relativistic, 394 f. Kirchhoff

diffraction, see Diffraction Kirchhoff's integral representation, 188 use of, ...

Ives-Stilwell experiment, 364 Jacobian, in

**Lorentz**transformation of coordinates,376 in transforming delta functions, 79 Kinematics, relativistic, 394 f. Kirchhoff

diffraction, see Diffraction Kirchhoff's integral representation, 188 use of, ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

8 other sections not shown

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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 modes 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