Classical Electrodynamics |
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Page 501
... motion . 14.6 Show explicitly by use of the Poisson sum formula or other means that , if the motion of a radiating particle repeats itself with periodicity T , the continuous frequency spectrum becomes a discrete spectrum containing ...
... motion . 14.6 Show explicitly by use of the Poisson sum formula or other means that , if the motion of a radiating particle repeats itself with periodicity T , the continuous frequency spectrum becomes a discrete spectrum containing ...
Page 581
... motion will be unimportant . The examples of the last two paragraphs show that the reactive effects of radiation on the motion of a charged particle can be expected to be important if the external forces are such that the motion changes ...
... motion will be unimportant . The examples of the last two paragraphs show that the reactive effects of radiation on the motion of a charged particle can be expected to be important if the external forces are such that the motion changes ...
Page 597
... motion . Nevertheless , the equation in its differential form contains unphysical behavior [ e.g. , solution ( 17.10 ) ] because it is higher order in time differentiation than a mechanical equation of motion should be . It is desirable ...
... motion . Nevertheless , the equation in its differential form contains unphysical behavior [ e.g. , solution ( 17.10 ) ] because it is higher order in time differentiation than a mechanical equation of motion should be . It is desirable ...
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