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... 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 v 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 v Fig . 13.3 e , m we may assume ...
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... impact parameters b less than this uncertainty , classical concepts fail ... parameter ( 13.6 ) . In the collision of two particles each one has a wave ... impact parameter is ( g ) = h ymv ( 13.40 ) For electrons incident on electrons we ...
... impact parameters b less than this uncertainty , classical concepts fail ... parameter ( 13.6 ) . In the collision of two particles each one has a wave ... impact parameter is ( g ) = h ymv ( 13.40 ) For electrons incident on electrons we ...
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... 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 ...
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