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Page 103
... Macroscopic Electrostatics ; Effects of Aggregates of Atoms The equations V.ε = : Απρ ' ▽ x € = 0 ( 4.20 ) govern electrostatic phenomena of all types , provided the ... Macroscopic Media , Dielectrics 103 Macroscopic electrostatics,
... Macroscopic Electrostatics ; Effects of Aggregates of Atoms The equations V.ε = : Απρ ' ▽ x € = 0 ( 4.20 ) govern electrostatic phenomena of all types , provided the ... Macroscopic Media , Dielectrics 103 Macroscopic electrostatics,
Page 194
... macroscopic displacement current Dat . The basic assumption inherent in our previous discussions was that the macroscopic fields E and B which satisfy the two homogeneous Maxwell's equations ( 6.28 ) are the averages of the ...
... macroscopic displacement current Dat . The basic assumption inherent in our previous discussions was that the macroscopic fields E and B which satisfy the two homogeneous Maxwell's equations ( 6.28 ) are the averages of the ...
Page 196
... macroscopic conduction - current density J ( x , t ) . Solutions ( 6.106 ) and ( 6.110 ) , augmented by the free ... macroscopic polarization P and magnetization M , the averaged charge and current densities in ( 6.111 ) can be expressed ...
... macroscopic conduction - current density J ( x , t ) . Solutions ( 6.106 ) and ( 6.110 ) , augmented by the free ... macroscopic polarization P and magnetization M , the averaged charge and current densities in ( 6.111 ) can be expressed ...
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