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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 In dErad 4 Zz2 m ( 2192M ) γ dEcoll 3π \ 137 / M In B ( 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 4 Zz2 m ( 2192M ) γ dEcoll 3π \ 137 / M In B ( 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 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