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Page 116
... molecule or group of molecules . But in dense media with closely packed molecules the polarization of neighboring molecules gives rise to an internal field E , at any given molecule in addition to the average macroscopic field E , so ...
... molecule or group of molecules . But in dense media with closely packed molecules the polarization of neighboring molecules gives rise to an internal field E , at any given molecule in addition to the average macroscopic field E , so ...
Page 117
John David Jackson. where SP is the contribution of molecules close to the given molecule , and ( 4/3 ) P is the contribution of the more distant molecules . It is customary to consider the two parts separately by imagining a spherical ...
John David Jackson. where SP is the contribution of molecules close to the given molecule , and ( 4/3 ) P is the contribution of the more distant molecules . It is customary to consider the two parts separately by imagining a spherical ...
Page 151
... molecule , and then average over molecules . The discussion proceeds exactly as in Section 5.6 for a localized current distribution . For a molecule with center at x , the vector potential at x is given approximately by amol ( x ) mmol ...
... molecule , and then average over molecules . The discussion proceeds exactly as in Section 5.6 for a localized current distribution . For a molecule with center at x , the vector potential at x is given approximately by amol ( x ) mmol ...
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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