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Page 299
... scattering of waves by an obstacle . We will consider the scattering of a plane electromagnetic wave by a perfectly conducting obstacle whose dimensions are large compared to a wavelength . For a thin , flat obstacle , the tech- niques ...
... scattering of waves by an obstacle . We will consider the scattering of a plane electromagnetic wave by a perfectly conducting obstacle whose dimensions are large compared to a wavelength . For a thin , flat obstacle , the tech- niques ...
Page 458
... scattering distribution for the projected 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 ) ...
... scattering distribution for the projected 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 ) ...
Page 459
... 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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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