dc.contributorMitskievich, N.V., Department of Physics, CUCEI, Universidad de Guadalajara, Apartado Postal 1-2011, Guadalajara, Jalisco, Mexico
dc.creatorMitskievich, N.V.
dc.date.accessioned2015-09-15T18:49:35Z
dc.date.accessioned2022-11-02T15:44:04Z
dc.date.available2015-09-15T18:49:35Z
dc.date.available2022-11-02T15:44:04Z
dc.date.created2015-09-15T18:49:35Z
dc.date.issued2008
dc.identifierhttp://www.scopus.com/inward/record.url?eid=2-s2.0-84892973172&partnerID=40&md5=2229eb12b9bb4fa0da2a68de0831b4ac
dc.identifierhttp://hdl.handle.net/20.500.12104/44176
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/5017783
dc.description.abstractThe Newtonian approximation in the gravitational field description not necessarily involves admission of non-relativistic properties of the source terms in Einstein's equations: it is sufficient to merely consider the weak-field condition for gravitational field. When, e.g., a source has electromagnetic nature, one simply cannot ignore its intrinsically rel-ativistic properties, since there cannot be invented any non-relativistic approximation which would adequately describe electromagnetic stress-energy tensor even at large distances where the fields become naturally weak. But the test particle on which gravitational field is acting, should be treated as non-relativistic (this premise is required for introduction of the Newtonian potential ?N from the geodesic equation). � 2008 World Scientific Publishing Co. Pte. Ltd.
dc.relationScopus
dc.relation11th Marcel Grossmann Meeting on Recent Developments in Theoretical and Experimental General Relativity, Gravitation and Relativistic Field Theories - Proc. of the MG11 Meeting on General Relativity
dc.relation2134
dc.relation2136
dc.titleRelativistic generalization of the inertial and gravitational masses equivalence principle
dc.typeConference Paper


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