Classical Electrodynamics |
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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 Hin and Bin by eliminating M : Bin + 2Hin = 3Bo ( 5.116 ) The hysteresis curve ...
... relation ( 5.87 ) and the phenomenon of hysteresis allow the creation of permanent magnets . We can solve equations ( 5.112 ) for one relation between Hin and Bin by eliminating M : Bin + 2Hin = 3Bo ( 5.116 ) The hysteresis curve ...
Page 346
... relation for small - amplitude longitudinal plasma oscillations is k2 • 42 - √k . V. fo do @p 2 = · V W ( b ) assuming that the phase velocity of the wave is large compared to thermal velocities , show that the dispersion relation ...
... relation for small - amplitude longitudinal plasma oscillations is k2 • 42 - √k . V. fo do @p 2 = · V W ( b ) assuming that the phase velocity of the wave is large compared to thermal velocities , show that the dispersion relation ...
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 ...
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Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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