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Page 181
... Lorentz condition . To see that potentials can always be Lorentz condition , suppose that the potentials A , and ( 6.33 ) do not satisfy ( 6.36 ) . Then let us make a gauge transformation to potentials A ' , ' and demand that A ...
... Lorentz condition . To see that potentials can always be Lorentz condition , suppose that the potentials A , and ( 6.33 ) do not satisfy ( 6.36 ) . Then let us make a gauge transformation to potentials A ' , ' and demand that A ...
Page 367
... Lorentz transfor- mation . If so , ( 11.45 ) would be correct as it stands . To see that the con- nection is more than a mere Lorentz transformation we note that the transformation from K ' to K " is equivalent to two successive Lorentz ...
... Lorentz transfor- mation . If so , ( 11.45 ) would be correct as it stands . To see that the con- nection is more than a mere Lorentz transformation we note that the transformation from K ' to K " is equivalent to two successive Lorentz ...
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... Lorentz condition , 181 in covariant form , 378 Lorentz force , 191 Lorentz force equation in covariant form , 405 Lorentz invariant , see Scalar , Relativ- istic invariance Lorentz line shape , 436 , 601 , 604 for cavity , 256 Lorentz ...
... Lorentz condition , 181 in covariant form , 378 Lorentz force , 191 Lorentz force equation in covariant form , 405 Lorentz invariant , see Scalar , Relativ- istic invariance Lorentz line shape , 436 , 601 , 604 for cavity , 256 Lorentz ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ