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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 354
... light source . No effect was observed which could be attributed to a change in the velocity of light due to the relative motion of the star and the earth . Another experiment on the light from rotating binary stars showed that the ...
... light source . No effect was observed which could be attributed to a change in the velocity of light due to the relative motion of the star and the earth . Another experiment on the light from rotating binary stars showed that the ...
Page 370
... light cone . The unshaded interior of the cone represents the past and the future , while the shaded region outside the cone is called " elsewhere . " A point inside ( outside ) the light cone is said to have a time - like ( space- like ) ...
... light cone . The unshaded interior of the cone represents the past and the future , while the shaded region outside the cone is called " elsewhere . " A point inside ( outside ) the light cone is said to have a time - like ( space- like ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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