On Mach's principle: Inertia as gravitation
| dc.creator | Martin, J. | |
| dc.creator | Ranada, Antonio F. | |
| dc.creator | Tiemblo, A. | |
| dc.date | 2007-03-28 | |
| dc.date.accessioned | 2026-07-07T07:54:13Z | |
| dc.date.available | 2026-07-07T07:54:13Z | |
| dc.description | In order to test the validity of Mach's principle, we calculate the action of the entire universe on a test mass in its rest frame, which is an acceleration ${\bf g}^*$. We show the dependence of the inertia principle on the lapse and the shift. Using the formalism of linearized gravitation, we obtain the non-relativistic limit of ${\bf g}^*$ in terms of two integrals. We follow then two approaches. In the first one, these integrals are calculated in the actual time section $t=t_0$ up to the distance $R_U=ct_0$. In the more exact and satisfactory second approach, they are calculated over the past light cone using the formalism of the retarded potentials. The aim is to find whether the acceleration $\dot{\bf v}$ in the LHS of Newton's second law can be interpreted as a reactive acceleration, in other words, as minus the acceleration of gravity ${\bf g}^*$ in the rest frame of the accelerated particle ({\it i. e.} to know whether or not ${\bf g}^*=-\dot{\bf v}$). The results strongly support Mach's idea since the reactive acceleration for $Ω_Λ=0.7$ turns out to be about ${\bf g}^*=-1.1 \dot{\bf v}$, in the first approach, and about ${\bf g}^*= -0.7 \dot{\bf v}$, in the second. These results depend little on $Ω_Λ$ if $Ω_Λ<0.9$. Even considering the approximations and idealizations made during the calculations, we deem these results as interesting and encouraging. | |
| dc.description | 17 pages, 2 figures | |
| dc.identifier | https://arxiv.org/abs/gr-qc/0703141 | |
| dc.identifier | http://arxiv.org/abs/gr-qc/0703141 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/126519 | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.title | On Mach's principle: Inertia as gravitation | |
| dc.type | text |