Classical ElectrodynamicsProblems after each chapter |
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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 ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ