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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 569
... Scattering of Electromagnetic Waves by a Conducting Sphere If a plane wave of electromagnetic radiation is incident on a spherical obstacle , as indicated schematically in Fig . 16.5 , it is scattered so that far away from the scatterer ...
... Scattering of Electromagnetic Waves by a Conducting Sphere If a plane wave of electromagnetic radiation is incident on a spherical obstacle , as indicated schematically in Fig . 16.5 , it is scattered so that far away from the scatterer ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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