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Page 348
... light in vacuum was equal to c . In other coordinate frames the velocity of light was presumably not c . To avoid setting electromagnetism apart from the rest of physics by a failure of Galilean relativity there are several avenues open ...
... light in vacuum was equal to c . In other coordinate frames the velocity of light was presumably not c . To avoid setting electromagnetism apart from the rest of physics by a failure of Galilean relativity there are several avenues open ...
Page 349
... light in liquids flowing in a pipe , both in the direction of and opposed to the propagation of the light . If the index of refraction of the liquid is n , then depending on which of the various hypotheses one chooses , he expects the ...
... light in liquids flowing in a pipe , both in the direction of and opposed to the propagation of the light . If the index of refraction of the liquid is n , then depending on which of the various hypotheses one chooses , he expects the ...
Page 362
... light . If the liquid has an index of refraction n we may assume that light propagates with a velocity u ' c / n relative to the liquid . From ( 11.28 ) the velocity of light observed in the laboratory is = น n H 1 ± ± v ( 1 -4 ) v nc ...
... light . If the liquid has an index of refraction n we may assume that light propagates with a velocity u ' c / n relative to the liquid . From ( 11.28 ) the velocity of light observed in the laboratory is = น n H 1 ± ± v ( 1 -4 ) v nc ...
Contents
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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