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Page 218
... perpendicular to the plane of incidence . E and H are continuous . In terms of fields ( 7.49 ) – ( 7.51 ) these boundary conditions at z = 0 are : [ ε ( Eo + Eo " ) ' E ' ] • n = 0 - x [ k x Eo + k " × E " - k ' × E ' ] . n = 0 ( Eo + ...
... perpendicular to the plane of incidence . E and H are continuous . In terms of fields ( 7.49 ) – ( 7.51 ) these boundary conditions at z = 0 are : [ ε ( Eo + Eo " ) ' E ' ] • n = 0 - x [ k x Eo + k " × E " - k ' × E ' ] . n = 0 ( Eo + ...
Page 314
... perpendicular to B. From ( 10.16 ) it is apparent that flow parallel to B is governed by the nonelectromagnetic forces alone . The velocity of flow of the fluid perpendicular to B , on the other hand , decays from some initially ...
... perpendicular to B. From ( 10.16 ) it is apparent that flow parallel to B is governed by the nonelectromagnetic forces alone . The velocity of flow of the fluid perpendicular to B , on the other hand , decays from some initially ...
Page 476
John David Jackson. parallel to and perpendicular to the velocity . But we have just seen that for comparable parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that ...
John David Jackson. parallel to and perpendicular to the velocity . But we have just seen that for comparable parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ