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Page 513
... radiative energy loss to collision energy loss ( 13.13 ) or ( 13.44 ) : dErad 4 Z m 22 dEcoll 3πT 137 M 2 1 In B. ( 15.27 ) For nonrelativistic particles ( v « c ) the radiative loss is completely negli- gible compared to the collision ...
... radiative energy loss to collision energy loss ( 13.13 ) or ( 13.44 ) : dErad 4 Z m 22 dEcoll 3πT 137 M 2 1 In B. ( 15.27 ) For nonrelativistic particles ( v « c ) the radiative loss is completely negli- gible compared to the collision ...
Page 580
... radiative effects begin to be important can thus be expressed by Erad ~ Eo ( 17.2 ) The specification of the ... radiative effects are unimportant . Only when the force is applied so suddenly and for such a short time that T ~ T will ...
... radiative effects begin to be important can thus be expressed by Erad ~ Eo ( 17.2 ) The specification of the ... radiative effects are unimportant . Only when the force is applied so suddenly and for such a short time that T ~ T will ...
Page 630
... radiative reaction , 597 Equations of motion with radiative re- action , 582 , 583 Ether , 347 Ether drift , experiment on , 349 Expansion , of circularly polarized plane wave , 569 of eikR / R , 541 of retarded quantity , 586 of scalar ...
... radiative reaction , 597 Equations of motion with radiative re- action , 582 , 583 Ether , 347 Ether drift , experiment on , 349 Expansion , of circularly polarized plane wave , 569 of eikR / R , 541 of retarded quantity , 586 of scalar ...
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Common terms and phrases
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