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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 acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ