Classical Electrodynamics |
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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 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 458
... scattering distribution for the projected angle of scattering is PM ( 0 ' ) d0 ' = 1 0,2 exp do ' TT ( 02 ) ( 02 ) ( 13.112 ) where both positive and negative values of ' are considered . The small- angle Rutherford formula ( 13.92 ) ...
... scattering distribution for the projected angle of scattering is PM ( 0 ' ) d0 ' = 1 0,2 exp do ' TT ( 02 ) ( 02 ) ( 13.112 ) where both positive and negative values of ' are considered . The small- angle Rutherford formula ( 13.92 ) ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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