Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 84
Page 456
... 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 457
... angle ) and mean square angle ( 02 ) given by ( 13.106 ) . Since the successive collisions are independent events , the central - limit theorem of statistics can be used to show that for a large number n of such collisions the ...
... angle ) and mean square angle ( 02 ) given by ( 13.106 ) . Since the successive collisions are independent events , the central - limit theorem of statistics can be used to show that for a large number n of such collisions the ...
Page 459
... 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 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ