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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 234
... relation , expressing the imaginary part as an integral over the real . ( b ) Show by direct calculation with the dispersion relation that in a frequency range where resonant absorption occurs there is necessarily anomalous dispersion ...
... relation , expressing the imaginary part as an integral over the real . ( b ) Show by direct calculation with the dispersion relation that in a frequency range where resonant absorption occurs there is necessarily anomalous dispersion ...
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 |
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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