Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 83
Page
... angle scattering . A particle traversing a finite thickness of matter will undergo very many small - angle deflections and will generally emerge at a small angle which is the cumu- lative statistical superposition of a large number of ...
... angle scattering . A particle traversing a finite thickness of matter will undergo very many small - angle deflections and will generally emerge at a small angle which is the cumu- lative statistical superposition of a large number of ...
Page
... angle increases linearly with the thickness t . But for reasonable thicknesses such that the particle does not lose appreciable energy , the Gaussian will still be peaked at very small forward angles . The multiple - scattering ...
... angle increases linearly with the thickness t . But for reasonable thicknesses such that the particle does not lose appreciable energy , the Gaussian will still be peaked at very small forward angles . The multiple - scattering ...
Page
... 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 ( 2 ) 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 ( 2 ) becomes comparable with the angle Omax ( 13.102 ) which limits ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
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