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. |
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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 ) -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 ) -m ] ...
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 ...
Page 413
... dipole moments vanish does the scattering fail to obey Rayleigh's law ; the scattering is then via quadrupole or higher multipoles ( or frequency- dependent dipole moments ) and varies as w ° or higher . Sometimes the dipole scattering ...
... dipole moments vanish does the scattering fail to obey Rayleigh's law ; the scattering is then via quadrupole or higher multipoles ( or frequency- dependent dipole moments ) and varies as w ° or higher . Sometimes the dipole scattering ...
Contents
L2 The Inverse Square Law or the Mass of the Photon | 1 |
1 | 17 |
1 | 27 |
Copyright | |
18 other sections not shown
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angle angular applied approximation assumed atomic average becomes boundary conditions calculate called Chapter charge charge density classical coefficients collision compared components conducting conductor consider constant coordinates corresponding cross section defined density dependence derivative determined dielectric dipole direction discussed distance distribution effects electric field electromagnetic electrons electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident induction inside integral involving limit linear Lorentz macroscopic magnetic field magnitude Maxwell means medium modes molecules momentum motion moving multipole normal observation obtained origin parallel particle physical plane polarization positive potential problem propagation properties quantum mechanics radiation radius region relation relative result satisfy scalar scattering shown solution space special relativity sphere spherical surface transformation unit vanishes vector velocity volume wave written zero