Classical ElectrodynamicsProblems after each chapter |
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... effects such as conduction and Hall effect are observed when fields are applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in ...
... effects such as conduction and Hall effect are observed when fields are applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in ...
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... 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 ...
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... 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 ...
... 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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ