Classical ElectrodynamicsThis edition refines and improves the first edition. It treats the present experimental limits on the mass of photon and the status of linear superposition, and introduces many other innovations. |
From inside the book
Results 1-3 of 85
Page 398
... dipole . This means that the magnetic induction for the present magnetic dipole source will be equal to the electric field for the electric dipole , with the substitution p → m . Thus we find eikr B = k2 ( nxm ) xn · + [ 3n ( n · m ) ...
... dipole . This means that the magnetic induction for the present magnetic dipole source will be equal to the electric field for the electric dipole , with the substitution p → m . Thus we find eikr B = k2 ( nxm ) xn · + [ 3n ( n · m ) ...
Page 408
... dipole moments ( 9.72 ) are only half as effective in producing a given amplitude as are the real dipole moments of a source located inside the guide . This can be pictured as because the effective dipoles of an aperture are in some ...
... dipole moments ( 9.72 ) are only half as effective in producing a given amplitude as are the real dipole moments of a source located inside the guide . This can be pictured as because the effective dipoles of an aperture are in some ...
Page 409
John David Jackson. ( d ) Effective Dipole Moments of Apertures On first encounter the effective dipole moments ( 9.72 ) are somewhat mysteri- ous . As already mentioned , they have a precise meaning in terms of the electric and magnetic ...
John David Jackson. ( d ) Effective Dipole Moments of Apertures On first encounter the effective dipole moments ( 9.72 ) are somewhat mysteri- ous . As already mentioned , they have a precise meaning in terms of the electric and magnetic ...
Contents
L2 The Inverse Square Law or the Mass of the Photon | 1 |
BoundaryValue Problems | 54 |
Multipoles Electrostatics | 136 |
Copyright | |
17 other sections not shown
Common terms and phrases
4-vector Ampère's law amplitude angle angular distribution angular momentum approximation atomic axis behavior boundary conditions calculate Chapter charge density charge q charged particle classical coefficients collision components conducting conductor consider coordinates cross section current density cylinder d³x defined dielectric constant diffraction dimensions dipole direction discussed electric and magnetic electric field electromagnetic fields electrons electrostatic expansion expression factor force frame frequency given Green function incident integral limit linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic monopole magnitude Maxwell equations medium modes molecules motion multipole multipole expansion multipole moments nonrelativistic normal obtained oscillations parallel parameter photon Phys plane wave plasma polarization problem propagation quantum quantum-mechanical radiation radius region relativistic result scattering shown in Fig sin² solution spectrum sphere spherical surface tensor theorem transverse unit V₁ vanishes vector potential velocity volume wave guide wave number wavelength written zero ΦΩ