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Page 315
... effects we treated the opposite quantities as given , but the equations are , of course , coupled . In the limit of very large conductivity it is convenient to relate the current density J in the force equation to the magnetic induction ...
... effects we treated the opposite quantities as given , but the equations are , of course , coupled . In the limit of very large conductivity it is convenient to relate the current density J in the force equation to the magnetic induction ...
Page 579
... effects . The remaining answer to the first question is that a completely satisfactory treatment of the reactive effects of radiation does not exist . The difficulties presented by this problem touch one of the most fundamental aspects ...
... effects . The remaining answer to the first question is that a completely satisfactory treatment of the reactive effects of radiation does not exist . The difficulties presented by this problem touch one of the most fundamental aspects ...
Page 580
... effects begin to be important can thus be expressed by Erad ~ Eo ( 17.2 ) The specification of the relevant energy E ... effects are unimportant . Only when the force is applied so suddenly and for such a short time that T ~ T will ...
... effects begin to be important can thus be expressed by Erad ~ Eo ( 17.2 ) The specification of the relevant energy E ... effects are unimportant . Only when the force is applied so suddenly and for such a short time that T ~ T will ...
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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