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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 J in a medium of unit permeability . 5.9 A circular loop of wire having a ... 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 J in a medium of unit permeability . 5.9 A circular loop of wire having a ... 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 ...
... 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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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