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Page 161
... relation ( 5.87 ) and the phenomenon of hysteresis allow the creation of permanent magnets . We can solve equations ( 5.112 ) for one relation between H and Bin by eliminating M : Bin + 2Hin = 3Bo ( 5.116 ) The hysteresis curve provides ...
... relation ( 5.87 ) and the phenomenon of hysteresis allow the creation of permanent magnets . We can solve equations ( 5.112 ) for one relation between H and Bin by eliminating M : Bin + 2Hin = 3Bo ( 5.116 ) The hysteresis curve provides ...
Page 346
... relation for small - amplitude longitudinal plasma oscillations is k . Vo fo k2 = d3v 2 k.v - w ( b ) assuming that the phase velocity of the wave is large compared to thermal velocities , show that the dispersion relation gives @ 2 ~ 1 ...
... relation for small - amplitude longitudinal plasma oscillations is k . Vo fo k2 = d3v 2 k.v - w ( b ) assuming that the phase velocity of the wave is large compared to thermal velocities , show that the dispersion relation gives @ 2 ~ 1 ...
Page 627
John David Jackson. Classical electron radius , 490 , 589 Clausius - Mossotti relation , 119 Closure , see Completeness relation Collisions , between charged particles as energy - loss mechanism , 430 relativistic kinematics of , 400 ...
John David Jackson. Classical electron radius , 490 , 589 Clausius - Mossotti relation , 119 Closure , see Completeness relation Collisions , between charged particles as energy - loss mechanism , 430 relativistic kinematics of , 400 ...
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