Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 69
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 1 0.2 PM ( 0 ' ) d0 ' = exp do ' - ( 02 ) ( 02 ( 13.112 ) where both positive and negative values of ' are considered . The small- angle Rutherford formula ( 13.92 ) can ...
... scattering distribution for the projected angle of scattering is 1 0.2 PM ( 0 ' ) d0 ' = exp do ' - ( 02 ) ( 02 ( 13.112 ) where both positive and negative values of ' are considered . The small- angle Rutherford formula ( 13.92 ) can ...
Page 459
... scattering distributions of projected angle . In the region of plural scattering ( ~ 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 ( ~ 2-3 ) the dotted curve indicates the smooth transition from the small - angle multiple scattering ( approximately Gaussian in shape ) to the wide ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
24 other sections not shown
Other editions - View all
Common terms and phrases
4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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