Classical ElectrodynamicsProblems after each chapter |
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Page 515
... cross section and the frequency . The radiation cross section has the dimensions of ( cross- sectional area ) ( energy ) ( frequency ) -1 . Since energy and frequency transform in the same way under Lorentz transformations , while ...
... cross section and the frequency . The radiation cross section has the dimensions of ( cross- sectional area ) ( energy ) ( frequency ) -1 . Since energy and frequency transform in the same way under Lorentz transformations , while ...
Page 525
... cross section ( 14.105 ) at low frequencies and the Klein - Nishina formula ( 14.106 ) at photon energies ho ' Mc2 . Thus , in the frame K ' , for frequencies small compared to Mc2 / h , the radiation cross section x ' ( w ' ) is given ...
... cross section ( 14.105 ) at low frequencies and the Klein - Nishina formula ( 14.106 ) at photon energies ho ' Mc2 . Thus , in the frame K ' , for frequencies small compared to Mc2 / h , the radiation cross section x ' ( w ' ) is given ...
Page 606
John David Jackson. We see that near the resonant frequency w the absorption cross section has the same Lorentz shape as the scattering cross section , but is larger by a factor г / г . At high frequencies → w2 , so that the absorption ...
John David Jackson. We see that near the resonant frequency w the absorption cross section has the same Lorentz shape as the scattering cross section , but is larger by a factor г / г . At high frequencies → w2 , so that the absorption ...
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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