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... scattering distribution for the projected angle of scattering is Pм ( 0 ' ) do ' = 1 0/2 exp - do ' 7 ( 02 ) ( 02 ) ( 13.112 ) where both positive and negative values of 0 ' are considered . The small- angle Rutherford formula ( 13.92 ) ...
... scattering distribution for the projected angle of scattering is Pм ( 0 ' ) do ' = 1 0/2 exp - do ' 7 ( 02 ) ( 02 ) ( 13.112 ) where both positive and negative values of 0 ' are considered . The small- angle Rutherford formula ( 13.92 ) ...
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... scattering distributions of projected angle . In the region of plural scattering ( a 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 ( a 2-3 ) the dotted curve indicates the smooth transition from the small - angle multiple scattering ( approximately Gaussian in shape ) to the wide ...
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... scattering cross section , but is larger by a factor / г . At high frequencies T → 2 , so that the absorption cross section approaches the constant Thomson value ( we have again ignored WT compared to unity ) . The absorption cross ...
... scattering cross section , but is larger by a factor / г . At high frequencies T → 2 , so that the absorption cross section approaches the constant Thomson value ( we have again ignored WT compared to unity ) . The absorption cross ...
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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