Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 71
Page 181
... Lorentz condition . To see that potentials can always be found to satisfy the Lorentz condition , suppose that the potentials A , Þ 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 , Þ which satisfy ( 6.32 ) and ( 6.33 ) do not satisfy ( 6.36 ) . Then let us make a gauge transformation to ...
Page 352
... Lorentz ( 1892 ) explained the null result while still retaining the ether concept by postulating that all material objects are contracted in their direction of motion as they move through the ether . The rule of contraction is - L ( v ) ...
... Lorentz ( 1892 ) explained the null result while still retaining the ether concept by postulating that all material objects are contracted in their direction of motion as they move through the ether . The rule of contraction is - L ( v ) ...
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 | |
24 other sections not shown
Other editions - View all
Common terms and phrases
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