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Page 315
... effects we treated the opposite quantities as given , but the equations are , of course , coupled . In the limit of very large conductivity it is convenient to relate the current density J in the force equation to the magnetic induction ...
... effects we treated the opposite quantities as given , but the equations are , of course , coupled . In the limit of very large conductivity it is convenient to relate the current density J in the force equation to the magnetic induction ...
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 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
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ