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Page 433
John David Jackson. Fig . 13.2 Energy transfer as a function of impact parameter . log △ E ( b ) - ΔΕ max bmin bmax ... impact parameters outside that interval , the energy transfer is considerably less . A fast particle passing through ...
John David Jackson. Fig . 13.2 Energy transfer as a function of impact parameter . log △ E ( b ) - ΔΕ max bmin bmax ... impact parameters outside that interval , the energy transfer is considerably less . A fast particle passing through ...
Page 434
... impact parameter b , measured from the origin O of the binding force , as shown in Fig . 13.3 . Since we are primarily interested in large impact parameters where binding effects are important , ze , M U Fig . 13.3 e , m we may assume ...
... impact parameter b , measured from the origin O of the binding force , as shown in Fig . 13.3 . Since we are primarily interested in large impact parameters where binding effects are important , ze , M U Fig . 13.3 e , m we may assume ...
Page 523
... impact parameters . This gives the energy per unit frequency interval present in the equivalent radiation field . As always in such problems we must specify a minimum impact parameter ... impact parameters greater than bmin the effects of the ...
... impact parameters . This gives the energy per unit frequency interval present in the equivalent radiation field . As always in such problems we must specify a minimum impact parameter ... impact parameters greater than bmin the effects of the ...
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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