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Page 456
... angle scattering . A particle traversing a finite thickness of matter will undergo very many small - angle deflections and will generally emerge at a small angle which is the cumu- lative statistical superposition of a large number of ...
... angle scattering . A particle traversing a finite thickness of matter will undergo very many small - angle deflections and will generally emerge at a small angle which is the cumu- lative statistical superposition of a large number of ...
Page 458
... angle of scattering is 1 0.2 PM ( 0 ' ) d0 ' = exp do ' - ( 02 ) ( 02 ( 13.112 ) where both positive and negative values of ' are considered . The small- angle Rutherford formula ( 13.92 ) can be expressed in terms of the pro- jected angle ...
... angle of scattering is 1 0.2 PM ( 0 ' ) d0 ' = exp do ' - ( 02 ) ( 02 ( 13.112 ) where both positive and negative values of ' are considered . The small- angle Rutherford formula ( 13.92 ) can be expressed in terms of the pro- jected angle ...
Page 459
... angles than a ~ 2.5 , and is somewhat more sharply peaked at zero angle than a Gaussian . On the other hand , if the thickness is great enough , the mean square angle ( 2 ) becomes comparable with the angle Omax ( 13.102 ) which limits ...
... angles than a ~ 2.5 , and is somewhat more sharply peaked at zero angle than a Gaussian . On the other hand , if the thickness is great enough , the mean square angle ( 2 ) becomes comparable with the angle Omax ( 13.102 ) which limits ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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