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Page 456
... Scattering and the Angular Distribution of Multiple Scattering Rutherford scattering is confined to very small angles even for a point Coulomb field , and for fast particles Omax is small compared to unity . Thus there is a very large ...
... Scattering and the Angular Distribution of Multiple Scattering Rutherford scattering is confined to very small angles even for a point Coulomb field , and for fast particles Omax is small compared to unity . Thus there is a very large ...
Page 459
... scattering distributions of projected angle . In the region of plural scattering ( ~ 2-3 ) the dotted curve indicates the smooth transition from the small - angle multiple scattering ( approximately Gaussian in shape ) to the wide ...
... scattering distributions of projected angle . In the region of plural scattering ( ~ 2-3 ) the dotted curve indicates the smooth transition from the small - angle multiple scattering ( approximately Gaussian in shape ) to the wide ...
Page 627
... Scattering Collision time , 507 for fields of relativistic particle , 382 Complementary screens , 288 Completeness relation , for Bessel func- tions on an infinite interval , 96 for complex exponentials , 47 , 84 for spherical harmonics ...
... Scattering Collision time , 507 for fields of relativistic particle , 382 Complementary screens , 288 Completeness relation , for Bessel func- tions on an infinite interval , 96 for complex exponentials , 47 , 84 for spherical harmonics ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ