Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 70
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 . T 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 ...
... motion will be unimportant . T 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 ...
Page 609
... motion in one dimension the equation of motion of Problem 17.4 can be written in the form , 2e2 p - - Pp2 3mc3 p2 + m2 c2 = 1 + p2 m2 c2f ( 7 ) where p is the momentum in the direction of motion , a dot means differentiation with ...
... motion in one dimension the equation of motion of Problem 17.4 can be written in the form , 2e2 p - - Pp2 3mc3 p2 + m2 c2 = 1 + p2 m2 c2f ( 7 ) where p is the momentum in the direction of motion , a dot means differentiation with ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ