THE MALTA COSMOLOGY TEMPLATE



Chapter 05 - Darkmatter






PARTS



Chapter
Home


Part 1
Centrifugal Blackholes


Part 2
Axial Blackholes


Part 3
Teelospheres as Darkmatter


Part 4
Selfproof
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Darkmatter Selfproofs

SELFPROOF O504 - STARS AT A GALACTIC CENTRE

CURRENT COSMOLOGY MODEL

The central parsec around Sagittarius A* contains thousands of stars. Although most of them are old red main-sequence stars, the Galactic Centre is also rich in massive stars. More than 100 OB and Wolf-Rayet stars have been identified there so far. They seem to have all been formed in a single star formation event a few million years ago. The existence of these relatively young (though evolved) stars was a surprise to experts, who expected the tidal forces from the central black hole to prevent their formation. This paradox of youth is even more remarkable for stars that are on very tight orbits around Sagittarius A*, such as S2. The scenarios invoked to explain this formation involve either star formation in a massive star cluster offset from the Galactic Centre that would have migrated to its current location once formed, or star formation within a massive, compact gas accretion disk around the central black hole. It is interesting to note that most of these 100 young, massive stars seem to be concentrated within one (according to the UCLA group) or two (according to the MPE group) disks, rather than randomly distributed within the central parsec. This observation however does not allow definite conclusions to be drawn on this point. (Wikipedia 6 Aug 2012)


MALTA COSMOLOGY TEMPLATE

  • Every blackhole in the Universe is within the gravitysheath of a larger object. (see Argument 0336)  
  • Many blackholes are within the teelospheres of larger objects. (see Argument 0337)  
  • Blackholes absorb teels from the teelosphere they are within which alters the blackhole's measures of mass and energy. (see Argument 0338)  
  • A stable blackhole within the teelosphere of a larger object becomes understable due to the differential absorption of mass and energy from the teelosphere. The stability of already overstable or understable blackholes alters commensurately. (see Argument 0339)  
  • A stable blackhole within a teelosphere, made understable through the differential absorption of mass and energy, ejects more than it absorbs until it returns to stability. The stability of already overstable or understable blackholes alters commensurately. (See Argument 0340)
COMMENTARY
  • The Sagittarius A* blackhole is the understable hub of a teelosphere that extends way beyond its disc of stars. The speed and density of this teelosphere decreases with distance from the surface of the blackhole per the Inverse Square Law. This means that within (say) half a parsec of the surface the teelstreams in the teelosphere are extremely dense and extremely fast. Any stars in this region are both marshalled by the teelstreams and subject to a constant absorption of teels from them.
  • Because the stars are constantly absorbing enormous quantities of very high realspeed teels, they are extremely understable, as are the particles they are made of. They are controlling their understability by ejecting enormous quantities of teels and photons but such is their rate of absorption that they can never stabilise until the blackhole itself comes nearer to stabilisation.
  • The net effect is that these stars do not age. Per the Current Cosmology Model, these are young stars but in practice they could be very old. Such is the battering they are receiving that, their brightness notwithstanding, they are probably quite diffuse and have a minimal fusion activity.
  • One consequence of the battering they are receiving is that each of the stars has its own extremely dense and extremely fast teelosphere which functions as a defensive shield. This is why these stars are able to cluster so closely together without either colliding or gravitationally tearing each other apart.
CONJECTURES FOR FURTHER RESEARCH
  • It may be that the number of stars clustering around the blackhole is conditioned by the mass of the blackhole in the same way that the number of electrons clustering around specific nuclei is controlled.
  • It may be that the blackhole's teelosphere conditions the mass and dimensions of the stars.
  • It may be that the markedly different nature of these stars, as compared to those only a short distance farther out, is because they are actually within the blackhole's teelocean.
  • It may be that, if the number of these stars is conditioned by the mass of the blackhole, if one star in the cluster decays for any reason it will be replaced by one of the stars from outside the cluster which is then “rejuvenated” by its dense teel battering.







Comments and suggestions:  peter.ed.winchester@gmail.com

Copyright 2013 Peter (Ed) Winchester



REVISIONS

03 Jul 2012 - Page revised to 3-section format.