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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 ( n x 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 ( n x Aẞ ) . This is perpendicular to n ( as it must be ) and can be resolved into components along and Thus nx ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ