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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 ...
... 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 ...
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 TT will radiative ...
... 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 TT will radiative ...
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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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