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Page 151
... atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions . To treat these atomic ...
... atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions . To treat these atomic ...
Page 443
... atom at a time , and then sum up incoherently the energy transfers to all the electrons in all the atoms with bmin < b < bmax . Now bmax is very large compared to atomic dimensions , especially for large y . Consequently in dense media ...
... atom at a time , and then sum up incoherently the energy transfers to all the electrons in all the atoms with bmin < b < bmax . Now bmax is very large compared to atomic dimensions , especially for large y . Consequently in dense media ...
Page 638
... atoms , 451 f . effect of atomic screening on , 453 effect of nuclear size on , 454 mean square angle of , 456 multiple , 458 single , 458 total atomic cross section for , 455 Scattering of radiation , by conducting sphere , at long ...
... atoms , 451 f . effect of atomic screening on , 453 effect of nuclear size on , 454 mean square angle of , 456 multiple , 458 single , 458 total atomic cross section for , 455 Scattering of radiation , by conducting sphere , at long ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ