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Page 103
... Macroscopic Electrostatics ; Effects of Aggregates of Atoms The equations V. • € = : Απρ ' ▽ × ε = 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. • € = : Απρ ' ▽ × ε = 0 ( 4.20 ) govern electrostatic phenomena of all types , provided the ... Macroscopic Media , Dielectrics 103 Macroscopic electrostatics,
Page 194
... macroscopic displacement current D / dt . 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 D / dt . 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 |
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