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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- ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ