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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 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 approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ