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 ) : 1 f = pE + J x B с ( 11.126 ) where J and p are the current and charge densities . Writing out a single ... volume , or the rate of change of mechanical energy of the sources per unit volume . Thus we see that the covariant ...
... volume ) : 1 f = pE + J x B с ( 11.126 ) where J and p are the current and charge densities . Writing out a single ... volume , or the rate of change of mechanical energy of the sources per unit volume . Thus we see that the covariant ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ