## 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

11.5 With the definition that x = [(v. x)w]|vo and x = x – x, equations (11.20) can be

combined to yield the general

? t;2 1 – = 1–3 1 x • W (11.21) r--H(-o) It should be noted that (11.21) represents ...

11.5 With the definition that x = [(v. x)w]|vo and x = x – x, equations (11.20) can be

combined to yield the general

**Lorentz**transformation:* x = x + –––. ** v--—w p? p? t;2 1 – = 1–3 1 x • W (11.21) r--H(-o) It should be noted that (11.21) represents ...

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 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

5 other sections not shown

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