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Page 433
John David Jackson. Fig . 13.2 Energy transfer as a function of impact parameter . log AE ( b ) -AE max bmin bmax log ... 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 AE ( b ) -AE max bmin bmax log ... 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 υ 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 υ Fig . 13.3 e , m we may assume ...
Page 514
... impact parameters . The relativistic contraction of the fields ( see Section 11.10 ) makes the col- lision time ( 11.120 ) smaller by a factor y = E / Mc2 . This means that the maximum impact parameter is increased from ( 15.14 ) to ...
... impact parameters . The relativistic contraction of the fields ( see Section 11.10 ) makes the col- lision time ( 11.120 ) smaller by a factor y = E / Mc2 . This means that the maximum impact parameter is increased from ( 15.14 ) to ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ