Jump to content

Shell collapsar

From Wikipedia, the free encyclopedia
This is an old revision of this page, as edited by Swen (talk | contribs) at 21:50, 21 December 2019 (Shuler corrected). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

A shell collapsar is a hypothetical compact astrophysical object, which might constitute an alternative explanation for observations of astronomical black hole candidates. It is a collapsed star that resembles a black hole, but is formed without a point-like central singularity and without an event horizon. The model of the shell collapsar was first proposed by Trevor W. Marshall[1] and allows the formation of neutron stars beyond the Tolman-Oppenheimer-Volkoff limit of 0.7 M☉.[2]

A shell collapsar is empty inside [3][3] and embodies the de-Sitter model there. According to Newton's shell theorem, the acceleration of gravity in the center of each celestial body is zero and rises to its surface (cf. gravitational field in the interior of the earth (PREM)). Without acceleration of gravity, the curvature of spacetime in the center of each celestial body is zero. With neutron stars beyond the Tolman-Oppenheimer-Volkoff limit, the time dilation due to gravity is extreme on its surface, so that the neutron star freezes on its outer shell.[4] [5] Another possible explanation is that when Newton's 1 / r² law is left, the Newtonian shell theorem no longer applies at the location of the strongest curvature, outward gravitational forces arise and pull the inner matter into the shell.[6] According to R.L. Shuler[7] this spacetime structure is determined by the entropy of the observable thermodynamics of real physical gravitational objects.

The shell collapsar is a special case of a gravastar. With the gravaster, an exotic form of matter stabilizes the object with the equation of state of dark energy inside. The shell collapsar comes to a similar result with ordinary neutron star matter and simply Einstein's field equations.

References

  1. ^ Marshall, Trevor (10.12.2016). "The Shell Collapsar—A Possible Alternative to Black Holes". Entropy. 18 (10): 363. doi:10.3390/e18100363. {{cite journal}}: Check date values in: |date= (help)CS1 maint: unflagged free DOI (link)
  2. ^ Marshall, Trevor. "Neutron stars beyond the TOV limit". Retrieved 09.24.2019. {{cite web}}: Check date values in: |accessdate= (help)
  3. ^ Mitra, Abhas (07.09.2013). "THE MASS OF THE OPPENHEIMER–SNYDER-BLACK HOLE: ONLY FINITE MASS QUASI-BLACK HOLES" (PDF). International Journal of Modern Physics D. 22 (9). doi:10.1142/S0218271813500545. {{cite journal}}: Check date values in: |date= (help)
  4. ^ Zakir, Zahid (11.02.2007). "General relativity constrains proper times and predicts frozen stars instead of black holes" (PDF). Theoretical Physics, Astrophysics and Cosmology: 1–8. doi:10.9751/TPAC.2497-006. {{cite journal}}: Check date values in: |date= (help)
  5. ^ Zakir, Zahid (01.12.2018). "On the consistency of the Oppenheimer-Snyder solution for a dust star. Reply to Marshall's criticism". Astrophysics and Space Science. 363 (2). doi:10.1007/s10509-018-3246-9. {{cite journal}}: Check date values in: |date= (help)
  6. ^ Marshall, Trevor W. "Supermassive neutron-star mergers as source of the gravitational wave events". Retrieved 12.21.2019. {{cite web}}: Check date values in: |accessdate= (help)
  7. ^ Shuler, Robert Luckett Jr. "Entropy-Like State Counting Leads to Human Readable Four Color Map Theorem Proof". Pure and Applied Mathematics Journal. 7 (3): 37. doi:10.11648/j.pamj.20180703.12.{{cite journal}}: CS1 maint: unflagged free DOI (link)