Classical ElectrodynamicsProblems after each chapter |
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Page 107
... volume of the molecules and the second being the polarization charge per unit volume . The presence of the divergence in the polarization - charge density seems very natural when one thinks of how this part of the charge density is ...
... volume of the molecules and the second being the polarization charge per unit volume . The presence of the divergence in the polarization - charge density seems very natural when one thinks of how this part of the charge density is ...
Page 190
... volume V is arbitrary , this can be cast into the form of a dif- ferential continuity equation or conservation law ... volume , plus the energy flowing out through the boundary surfaces of the volume per unit time , is equal to the ...
... volume V is arbitrary , this can be cast into the form of a dif- ferential continuity equation or conservation law ... volume , plus the energy flowing out through the boundary surfaces of the volume per unit time , is equal to the ...
Page 384
... volume ) : f = pE + - J x B J × B 1 / C ( 11.126 ) where J and p are the current and charge densities . Writing out ... volume , or the rate of change of mechanical energy of the sources per unit volume . Thus we see that the covariant ...
... volume ) : f = pE + - J x B J × B 1 / C ( 11.126 ) where J and p are the current and charge densities . Writing out ... volume , or the rate of change of mechanical energy of the sources per unit volume . Thus we see that the covariant ...
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Common terms and phrases
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