Classical ElectrodynamicsProblems after each chapter |
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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 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 ) ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ