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Page 352
... relative velocity of 106 cm / sec would have been seen ( i.e. , one - third of the above estimate ) . No fringe shift was found . Since the original work of Michelson the experiment has been repeated many times with modifi- cations such ...
... relative velocity of 106 cm / sec would have been seen ( i.e. , one - third of the above estimate ) . No fringe shift was found . Since the original work of Michelson the experiment has been repeated many times with modifi- cations such ...
Page 356
... relative motion of K and K ' is parallel to the z axis . It is a straight - forward matter to write down the result for an arbitrary velocity v of translation of K ' relative to K , as shown in Fig . 11.5 . Equation ( 11.19 ) clearly ...
... relative motion of K and K ' is parallel to the z axis . It is a straight - forward matter to write down the result for an arbitrary velocity v of translation of K ' relative to K , as shown in Fig . 11.5 . Equation ( 11.19 ) clearly ...
Page 358
... relative concept . Another consequence of the special theory of relativity is time dilatation . A clock moving relative to an observer is found to run more slowly than one at rest relative to him . The most fundamental " clocks " which ...
... relative concept . Another consequence of the special theory of relativity is time dilatation . A clock moving relative to an observer is found to run more slowly than one at rest relative to him . The most fundamental " clocks " which ...
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