Classical Electrodynamics |
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Page 392
... particles behave kinematically in the same way , whether charged or neutral . A charged particle can be thought of as a very localized distribution of charge and mass . To find the force acting on such a particle we integrate the ...
... particles behave kinematically in the same way , whether charged or neutral . A charged particle can be thought of as a very localized distribution of charge and mass . To find the force acting on such a particle we integrate the ...
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 506
... charged particle initially at rest to some final velocity in a very short time interval , or , alternatively , as the sudden switching on of the charge of the moving particle in the same short interval . We will discuss nuclear beta ...
... charged particle initially at rest to some final velocity in a very short time interval , or , alternatively , as the sudden switching on of the charge of the moving particle in the same short interval . We will discuss nuclear beta ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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