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Page 407
... nonrelativistic motion shows that λ = mc2 , yielding the free - particle Lagrangian ( 12.69 ) . 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 ) . The general requirement that yL be Lorentz invariant allows us to determine the Lagrangian for a relativistic charged particle in external ...
Page 509
... nonrelativistic small- angle collisions . They have been verified in detail for the continuous X - ray spectrum produced by electrons of kinetic energies in the kilovolt range . It is evident that the sum of the two intensities is ...
... nonrelativistic small- angle collisions . They have been verified in detail for the continuous X - ray spectrum produced by electrons of kinetic energies in the kilovolt range . It is evident that the sum of the two intensities is ...
Page 517
... nonrelativistic ( relativistic ) limiting form . When < w , the argument of the logarithm in the radiation cross ... nonrelativistic limit . A typical figure is w / wmax 0.07 for electrons of 100 - Kev kinetic energy incident on a gold ...
... nonrelativistic ( relativistic ) limiting form . When < w , the argument of the logarithm in the radiation cross ... nonrelativistic limit . A typical figure is w / wmax 0.07 for electrons of 100 - Kev kinetic energy incident on a gold ...
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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