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Page 222
... light without loss in intensity . In nuclear physics Lucite or other plastic " light pipes " are used to carry light emitted from a scintillation crystal because of the passage of an ionizing particle to a photomultiplier tube , where ...
... light without loss in intensity . In nuclear physics Lucite or other plastic " light pipes " are used to carry light emitted from a scintillation crystal because of the passage of an ionizing particle to a photomultiplier tube , where ...
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 is determined by the transmitting medium ( our atmosphere in this case ) or that the ether is dragged along by the earth . In neither case would aberration occur . Fizeau's experiment involved measuring , by means of an ...
... light is determined by the transmitting medium ( our atmosphere in this case ) or that the ether is dragged along by the earth . In neither case would aberration occur . Fizeau's experiment involved measuring , by means of an ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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