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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 ...
Page 508
... perpendicular to the plane containing ẞ , and n . The direction of polarization of the radiation is given by the vector nx ( nx Aẞ ) . This is perpendicular to n ( as it must be ) and can be resolved into components along and Thus nx ...
... perpendicular to the plane containing ẞ , and n . The direction of polarization of the radiation is given by the vector nx ( nx Aẞ ) . This is perpendicular to n ( as it must be ) and can be resolved into components along and Thus nx ...
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