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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 374
11.12 Time dilatation and FitzGerald - Lorentz contraction in terms of a rotation of
space - time axes . It 3 in agreement with ( 11.22 ) . Similarly the time intervals T ,
in the frame K ' are seen in the frame K as intervals T , where T = T , cos y = yT ...
11.12 Time dilatation and FitzGerald - Lorentz contraction in terms of a rotation of
space - time axes . It 3 in agreement with ( 11.22 ) . Similarly the time intervals T ,
in the frame K ' are seen in the frame K as intervals T , where T = T , cos y = yT ...
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 , in ...
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 , in ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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