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Page 132
... magnet date from before 1600. In contrast to electrostatics , the basic laws of magnetic fields did not follow straightforwardly from man's earliest contact with magnetic materials . The reasons are several , but they all stem from the ...
... magnet date from before 1600. In contrast to electrostatics , the basic laws of magnetic fields did not follow straightforwardly from man's earliest contact with magnetic materials . The reasons are several , but they all stem from the ...
Page 133
... magnetic induction ) , we have a more complicated situation than for the electric field . Further quantitative elucidation of magnetic phenomena did not occur until the connection between currents and magnetic fields was established . A ...
... magnetic induction ) , we have a more complicated situation than for the electric field . Further quantitative elucidation of magnetic phenomena did not occur until the connection between currents and magnetic fields was established . A ...
Page 633
... Magnet , permanent , 161 , 167 Magnetic dipole , see Dipole fields , Di- pole moment Magnetic field H , boundary conditions on , 154 definition of macroscopic , 153 see also Magnetic induction Magnetic flux density , see Magnetic in- ...
... Magnet , permanent , 161 , 167 Magnetic dipole , see Dipole fields , Di- pole moment Magnetic field H , boundary conditions on , 154 definition of macroscopic , 153 see also Magnetic induction Magnetic flux density , see Magnetic in- ...
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Common terms and phrases
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