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Page 429
John David Jackson. 13 Collisions between Charged Particles , Energy Loss , and Scattering In this chapter collisions between swiftly moving , charged particles are considered , with special emphasis on the exchange of energy between ...
John David Jackson. 13 Collisions between Charged Particles , Energy Loss , and Scattering In this chapter collisions between swiftly moving , charged particles are considered , with special emphasis on the exchange of energy between ...
Page 463
... collisions of a fast , but nonrelativistic , heavy particle of charge ze passing through an electronic plasma . Assume that the screened Coulomb interaction ( 10.113 ) acts between the electrons and the incident particle . ( a ) Show ...
... collisions of a fast , but nonrelativistic , heavy particle of charge ze passing through an electronic plasma . Assume that the screened Coulomb interaction ( 10.113 ) acts between the electrons and the incident particle . ( a ) Show ...
Page 536
... collisions can be divided into two kinds : close collisions where the particle passes through the atom ( b d ) , and distant collisions > where the particle passes by outside the atom ( b > d ) . The atomic “ radius " d can be taken as ...
... collisions can be divided into two kinds : close collisions where the particle passes through the atom ( b d ) , and distant collisions > where the particle passes by outside the atom ( b > d ) . The atomic “ radius " d can be taken as ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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