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... radiative energy loss as V -x 16 NZ ( 2 ) = ( ' In ( 1 + √1 ) dz dErad dx == 3 Ze2 ze 244 1 Mc2 x dx ( 15.26 ) The dimensionless integral has the value unity . For comparison we write the ratio of radiative energy loss to collision ...
... radiative energy loss as V -x 16 NZ ( 2 ) = ( ' In ( 1 + √1 ) dz dErad dx == 3 Ze2 ze 244 1 Mc2 x dx ( 15.26 ) The dimensionless integral has the value unity . For comparison we write the ratio of radiative energy loss to collision ...
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... 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 TT 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 TT will ...
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... 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 ...
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