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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 450
John David Jackson. 13.5 Energy Loss in an Electronic Plasma The loss of energy by a nonrelativistic particle passing through a plasma can be treated in a manner similar to the density effect for a relativistic particle . As was ...
John David Jackson. 13.5 Energy Loss in an Electronic Plasma The loss of energy by a nonrelativistic particle passing through a plasma can be treated in a manner similar to the density effect for a relativistic particle . As was ...
Page 519
... loss to collision loss now becomes In dErad dEcoll 4 Zz2 m ( 2192 2192M 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 for lead ...
... loss to collision loss now becomes In dErad dEcoll 4 Zz2 m ( 2192 2192M 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 for lead ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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