Classical Electrodynamics |
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Page 407
... nonrelativistic motion shows that λ = mc2 , yielding the free - particle Lagrangian ( 12.69 ) . 2 The general requirement that yL be Lorentz invariant allows us to determine the Lagrangian for a relativistic charged particle in external ...
... nonrelativistic motion shows that λ = mc2 , yielding the free - particle Lagrangian ( 12.69 ) . 2 The general requirement that yL be Lorentz invariant allows us to determine the Lagrangian for a relativistic charged particle in external ...
Page 505
... nonrelativistic and relativistic charged particles in external fields were treated . The present chapter is devoted to problems of emission of electromagnetic radiation by charged particles in atomic and nuclear processes . Particles ...
... nonrelativistic and relativistic charged particles in external fields were treated . The present chapter is devoted to problems of emission of electromagnetic radiation by charged particles in atomic and nuclear processes . Particles ...
Page 517
... nonrelativistic ( relativistic ) limiting form . When w < ∞ , the argument of the logarithm in the radiation cross ... nonrelativistic limit . A typical figure is ws / wmax 0.07 for electrons of 100 - Kev kinetic energy incident on a ...
... nonrelativistic ( relativistic ) limiting form . When w < ∞ , the argument of the logarithm in the radiation cross ... nonrelativistic limit . A typical figure is ws / wmax 0.07 for electrons of 100 - Kev kinetic energy incident on a ...
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