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Page 116
... molecule is E + E ,. The internal field can be written as E ; = ( 4 + S ) P 3 ( 4.67 ) where SP is the contribution of molecules close to the. 116 Classical Electrodynamics Molecular polarizability and electric susceptibility,
... molecule is E + E ,. The internal field can be written as E ; = ( 4 + S ) P 3 ( 4.67 ) where SP is the contribution of molecules close to the. 116 Classical Electrodynamics Molecular polarizability and electric susceptibility,
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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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