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Page 448
... loss for ultrarelativistic particles pro- vided their densities are such that the density of electrons is the same in each . Since there are numerous calculated curves of energy loss based on Bethe's formula ( 13.44 ) , it is often ...
... loss for ultrarelativistic particles pro- vided their densities are such that the density of electrons is the same in each . Since there are numerous calculated curves of energy loss based on Bethe's formula ( 13.44 ) , it is often ...
Page 449
... loss , including the density effect . The dotted curve is the total energy loss without density correction . The solid curves have the density effect incorporated , the upper one being the total energy loss and the lower one the energy ...
... loss , including the density effect . The dotted curve is the total energy loss without density correction . The solid curves have the density effect incorporated , the upper one being the total energy loss and the lower one the energy ...
Page 519
... loss to collision loss now becomes dErad dEcoll ལ In 4 Zz2 m ( 123m ( 2192M Zm γ 3π 137 / M In Ba ( 15.46 ) The value of y for which this ratio is unity depends on the particle and on Z. For electrons it is y ~ 200 for air and y ~ 20 ...
... loss to collision loss now becomes dErad dEcoll ལ In 4 Zz2 m ( 123m ( 2192M Zm γ 3π 137 / M In Ba ( 15.46 ) The value of y for which this ratio is unity depends on the particle and on Z. For electrons it is y ~ 200 for air and y ~ 20 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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