Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 78
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 ...
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 | |
21 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ