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Page 457
... angle of scattering 0 ' , the projection being made on some convenient plane such as the plane of a photographic ... angle ) and mean square angle ( 02 ) given by ( 13.106 ) . Since the successive collisions are independent events , the ...
... angle of scattering 0 ' , the projection being made on some convenient plane such as the plane of a photographic ... angle ) and mean square angle ( 02 ) given by ( 13.106 ) . Since the successive collisions are independent events , the ...
Page 458
... angle of scattering is 1 0'2 PM ( 0 ' ) d0 ' = exp do ' ( 02 ) Vπ ( 02 ( 13.112 ) where both positive and negative values of 0 ' are considered . The small- angle Rutherford formula ( 13.92 ) can be expressed in terms of the pro- jected ...
... angle of scattering is 1 0'2 PM ( 0 ' ) d0 ' = exp do ' ( 02 ) Vπ ( 02 ( 13.112 ) where both positive and negative values of 0 ' are considered . The small- angle Rutherford formula ( 13.92 ) can be expressed in terms of the pro- jected ...
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 ( O2 ) 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 ( O2 ) becomes comparable with the angle Omax ( 13.102 ) which limits ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ