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Page 116
... molecular separations are large there is little difference between the macroscopic field and that acting on any molecule or group of molecules . But in dense media with closely packed molecules the polarization of neighboring molecules ...
... molecular separations are large there is little difference between the macroscopic field and that acting on any molecule or group of molecules . But in dense media with closely packed molecules the polarization of neighboring molecules ...
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 ) ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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