Relativistic generalization of the inertial and gravitational masses equivalence principle
| dc.creator | Mitskievich, Nikolai V. | |
| dc.date | 2006-11-03 | |
| dc.date.accessioned | 2026-07-07T07:31:54Z | |
| dc.date.available | 2026-07-07T07:31:54Z | |
| dc.description | The Newtonian approximation for the gravitational field equation should not necessarily involve 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 a source has electromagnetic nature, one simply {\em cannot} ignore its intrinsically relativistic properties, since there cannot be invented any non-relativistic approximation which would describe electromagnetic stress-energy tensor adequately, 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 $Φ_{\rm N}$ from the geodesic equation). | |
| dc.description | 5 pages, a talk delivered at the 11th Marcel Grossmann Meeting (Session GT4), Berlin, 2006 | |
| dc.identifier | https://arxiv.org/abs/gr-qc/0611017 | |
| dc.identifier | http://arxiv.org/abs/gr-qc/0611017 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/118919 | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.title | Relativistic generalization of the inertial and gravitational masses equivalence principle | |
| dc.type | text |