Classical Electrodynamics |
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Page 181
... Lorentz condition . To see that potentials can always be found to satisfy the Lorentz condition , suppose that the potentials A , D which satisfy ( 6.32 ) and ( 6.33 ) do not satisfy ( 6.36 ) . Then let us make a gauge transformation to ...
... Lorentz condition . To see that potentials can always be found to satisfy the Lorentz condition , suppose that the potentials A , D which satisfy ( 6.32 ) and ( 6.33 ) do not satisfy ( 6.36 ) . Then let us make a gauge transformation to ...
Page 357
... Lorentz transformation : * x ' = x + 1 X.V v2 V 1 vt = - c2 - | " — X.V c2 ( 11.21 ) 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 ...
... Lorentz transformation : * x ' = x + 1 X.V v2 V 1 vt = - c2 - | " — X.V c2 ( 11.21 ) 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 ...
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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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