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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 439
... collision is incorrect . But if we consider a large number of collisions , we find that on the average a small amount of energy is transferred . It is not transferred in every collision , however . In most collisions no energy is ...
... collision is incorrect . But if we consider a large number of collisions , we find that on the average a small amount of energy is transferred . It is not transferred in every collision , however . In most collisions no energy is ...
Page 443
... collisions , but will be valid for the great bulk of the collisions . The problem of finding the electric field in the medium [ Sect . 13.4 ] 443 Collisions between Charged Particles Density effect in collision energy loss,
... collisions , but will be valid for the great bulk of the collisions . The problem of finding the electric field in the medium [ Sect . 13.4 ] 443 Collisions between Charged Particles Density effect in collision energy loss,
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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