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Page 233
... Show that plane waves with frequency @ and wave vector k must satisfy @ 2 kx ( k × E ) + D = 0 ( b ) Show that for a given wave vector k = kn there are two distinct modes of propagation with different phase velocities v = w / k which ...
... Show that plane waves with frequency @ and wave vector k must satisfy @ 2 kx ( k × E ) + D = 0 ( b ) Show that for a given wave vector k = kn there are two distinct modes of propagation with different phase velocities v = w / k which ...
Page 365
... shows why the doublets are " inverted " in nuclei . The Uhlenbeck - Goudsmit hypothesis was that an electron possessed a spin angular momentum S ( which could take on quantized values of ± ħ / 2 along any axis ) and a magnetic moment μ ...
... shows why the doublets are " inverted " in nuclei . The Uhlenbeck - Goudsmit hypothesis was that an electron possessed a spin angular momentum S ( which could take on quantized values of ± ħ / 2 along any axis ) and a magnetic moment μ ...
Page 367
... show that the time variables in K " and K ' are related by 1 " = t ' - x ' c2 1 1 δν δν + 1 ( 11.50 ) v2 v2 correct to first order in dv . This shows that the direct transformation from K ' to K " involves an infinitesimal Lorentz ...
... show that the time variables in K " and K ' are related by 1 " = t ' - x ' c2 1 1 δν δν + 1 ( 11.50 ) v2 v2 correct to first order in dv . This shows that the direct transformation from K ' to K " involves an infinitesimal Lorentz ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ