Classical Electrodynamics |
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Page 181
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) ...
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 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 ...
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 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, ...
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 |
References and suggested reading | 50 |
Copyright | |
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