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Page 309
... effects such as conduction and Hall effect are observed when fields are applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in ...
... effects such as conduction and Hall effect are observed when fields are applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in ...
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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ