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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,
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ