Classical Electrodynamics |
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Page 579
... effects . The remaining answer to the first question is that a completely satisfactory treatment of the reactive effects of radiation does not exist . The difficulties presented by this problem touch one of the most fundamental aspects ...
... effects . The remaining answer to the first question is that a completely satisfactory treatment of the reactive effects of radiation does not exist . The difficulties presented by this problem touch one of the most fundamental aspects ...
Page 580
... effects begin to be important can thus be expressed by Erad ~ Eo ( 17.2 ) The specification of the relevant energy E ... effects are unimportant . Only when the force is applied so suddenly and for such a short time that T ~ will ...
... effects begin to be important can thus be expressed by Erad ~ Eo ( 17.2 ) The specification of the relevant energy E ... effects are unimportant . Only when the force is applied so suddenly and for such a short time that T ~ will ...
Page 581
... effects are sufficiently small that they have a negligible effect on the short - term motion . Their long - term , cumulative effects can be taken into account in an approximate way , as we will see immediately . 17.2 Radiative Reaction ...
... effects are sufficiently small that they have a negligible effect on the short - term motion . Their long - term , cumulative effects can be taken into account in an approximate way , as we will see immediately . 17.2 Radiative Reaction ...
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