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Page 133
John David Jackson. Already , in the definition of the magnetic - flux density B ( sometimes called the magnetic induction ) , we have a more complicated situation than for the electric field . Further quantitative elucidation of magnetic ...
John David Jackson. Already , in the definition of the magnetic - flux density B ( sometimes called the magnetic induction ) , we have a more complicated situation than for the electric field . Further quantitative elucidation of magnetic ...
Page 167
... magnetic induction appears to be due to a 2μ μ + J in a medium of unit permeability . 5.9 A circular loop of wire ... magnetic field H and magnetic induction B at all points on the axis of the cylinder , both inside and outside . ( b ) ...
... magnetic induction appears to be due to a 2μ μ + J in a medium of unit permeability . 5.9 A circular loop of wire ... magnetic field H and magnetic induction B at all points on the axis of the cylinder , both inside and outside . ( b ) ...
Page 170
... magnetic fields were made by Faraday ( 1831 ) in experiments on the behavior of currents in circuits placed in time ... induction in the neighborhood of the circuit is B. The magnetic flux linking the circuit is defined by F = B. B⚫n da ...
... magnetic fields were made by Faraday ( 1831 ) in experiments on the behavior of currents in circuits placed in time ... induction in the neighborhood of the circuit is B. The magnetic flux linking the circuit is defined by F = B. B⚫n da ...
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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