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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 ) ...
... 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 ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ