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Shell collapsar

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This is an old revision of this page, as edited by Maxwallis (talk | contribs) at 23:52, 21 February 2025 (Omit repetition of Newon's shell heorem (which is hardly relevant); check on Zakir's paper to represent them more accurately). 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. Being of neutron star size (~11km), it strongly distorts light rays like a black hole, but has no central point-like singularity. Matter has collapsed onto the event horizon forming a shell there of ultra-high density. 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 2.1 M☉.[2]

A shell collapsar is void inside[3] apart from intense gravitational field energy there. Newton's shell theorem does not apply, but Einsteinian gravitation in the highly non-linear regime. . Gravitational time dilation is extreme on its surface (just outside the event horizon), so that the accreting neutron matter freezes onto the outer shell, as described in the ‘frozar’ model[4][5] Zakir conceives that outward gravitational forces arise in the interior and push inner matter into the ‘frozar’ shell.[6]

The shell collapsar is a special case of a gravastar. With the gravastar, 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 describing intense gravitational energy density, comparable as E/c² to the neutron matter density.

References

  1. ^ Marshall, Trevor (2016). "The Shell Collapsar—A Possible Alternative to Black Holes". Entropy. 18 (10): 363. Bibcode:2016Entrp..18..363M. doi:10.3390/e18100363.
  2. ^ Marshall, Trevor. "Neutron stars beyond the TOV limit". Retrieved 2019-12-21.
  3. ^ Mitra, Abhas (2013). "The Mass of the Oppenheimer–Snyder-Black Hole: Only Finite Mass Quasi-Black Holes". International Journal of Modern Physics D. 22 (9): 1350054. doi:10.1142/S0218271813500545.
  4. ^ Zakir, Zahid (2007). "General relativity constrains proper times and predicts frozen stars instead of black holes". Theoretical Physics, Astrophysics and Cosmology: 1–8. arXiv:0705.2585. doi:10.9751/TPAC.2497-006.
  5. ^ Zakir, Zahid (2018). "On the consistency of the Oppenheimer-Snyder solution for a dust star. Reply to Marshall's criticism". Astrophysics and Space Science. 363 (2): 30. Bibcode:2018Ap&SS.363...30Z. doi:10.1007/s10509-018-3246-9.
  6. ^ Marshall, Trevor W. "Supermassive neutron-star mergers as source of the gravitational wave events". Retrieved 2019-12-21.