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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 current distribution 2μ μ + 1 i ) J in a medium of unit permeability . 5.9 A circular loop of wire having a radius a and carrying a current I is located in vacuum with its center a distance d ...
... magnetic induction appears to be due to a current distribution 2μ μ + 1 i ) J in a medium of unit permeability . 5.9 A circular loop of wire having a radius a and carrying a current I is located in vacuum with its center a distance d ...
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.nda ...
... 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.nda ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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