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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
... 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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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