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Page 181
John David Jackson. 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 ...
John David Jackson. 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 ...
Page 372
... transformations in four dimensions . The Lorentz transformation ( 11.21 ) can be written in the general form : = Σαμώνη μ = 1 , 2 , 3 , 4 v = 1 ( 11.70 ) where the coefficients a , are constants characteristic of the particular ...
... transformations in four dimensions . The Lorentz transformation ( 11.21 ) can be written in the general form : = Σαμώνη μ = 1 , 2 , 3 , 4 v = 1 ( 11.70 ) where the coefficients a , are constants characteristic of the particular ...
Page 373
... transformation ( 11.19 ) . The formal representation of transformation ( 11.75 ) as a rotation of axes in the x , x plane ( with x , drawn as if it were real ) can be accomplished simply . Figure 11.11 shows a rotation of the axes ...
... transformation ( 11.19 ) . The formal representation of transformation ( 11.75 ) as a rotation of axes in the x , x plane ( with x , drawn as if it were real ) can be accomplished simply . Figure 11.11 shows a rotation of the axes ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ