## Classical Electrodynamics |

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Page 181

6.5 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 (6.36) ...

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 (6.36) ...

Page 357

John David Jackson, Patrick Thaddeus Jackson. Fig. 11.5 With the definition that

x = [(v. x)v]|v° and x, - x -x, equations (11.20) can be combined to yield the

general

co 1 z ...

John David Jackson, Patrick Thaddeus Jackson. Fig. 11.5 With the definition that

x = [(v. x)v]|v° and x, - x -x, equations (11.20) can be combined to yield the

general

**Lorentz**transformation:* x = x + –––1 *** –––v U” p? p? 1 — – 1 — — coco 1 z ...

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 |

BoundaryValue Problems in Electrostatics II | 54 |

Copyright | |

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