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Jefimenko's equations : ウィキペディア英語版 | Jefimenko's equations
In electromagnetism, Jefimenko's equations (named after Oleg D. Jefimenko) describe the behavior of the electric and magnetic fields in terms of the charge and current distributions at retarded times. Jefimenko's equations〔Oleg D. Jefimenko, ''Electricity and Magnetism: An Introduction to the Theory of Electric and Magnetic Fields'', Appleton-Century-Crofts (New-York - 1966). 2nd ed.: Electret Scientific (Star City - 1989), ISBN 978-0-917406-08-9. See also: David J. Griffiths, Mark A. Heald, ''Time-dependent generalizations of the Biot–Savart and Coulomb laws'', American Journal of Physics 59 (2) (1991), 111-117.〕 are the solution of Maxwell's equations for an assigned distribution of electric charges and currents, under the assumption that there is no electromagnetic field other than the one produced by those charges and currents, that is no electromagnetic field coming from the infinite past. == Equations ==
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