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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 357
... Lorentz transformation : * 1 x ' = x + X.V v2 x . " ) 1 vt ( 11.21 ) - c2 It should be noted that ( 11.21 ) represents a single Lorentz transformation to a reference frame K ' moving with velocity v relative to the system K. Successive ...
... Lorentz transformation : * 1 x ' = x + X.V v2 x . " ) 1 vt ( 11.21 ) - c2 It should be noted that ( 11.21 ) represents a single Lorentz transformation to a reference frame K ' moving with velocity v relative to the system K. Successive ...
Page 632
... 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 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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