THE MALTA COSMOLOGY TEMPLATE



Chapter 3 - Blackholes






PARTS



Chapter
Home


Part 1
Teelpairs


Part 2
Blackholes


Part 3
Blackhole structure


Part 4
Blackhole mechanics


Part 5
Blackhole selfstabilisation


Part 6
Blackhole gravitational attunement


Part 7
Blackhole teelospheric attunement


Part 8
Selfproof

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Part 8 - Selfproof (cont)

SELFPROOF 0304 - EXTREMAL BLACKHOLE


CURRENT COSMOLOGY MODEL



An extremal blackhole is a blackhole with the minimal possible mass that can be compatible with a given charge and angular momentum. In other words, this is the smallest possible blackhole that can exist while rotating at a given fixed constant speed. The concept of an extremal blackhole is theoretical and none have thus far been observed in nature. However, many theories are based on their existence. (Wikipedia 24 Jan 2012)



MALTA COSMOLOGY TEMPLATE


  • A blackhole consists of a minimum of three teels matrixed to each other as three stable/overstable teelpairs. (see Argument 0312)  
  • Every blackhole has a vergence velocity.  (see Argument 0315)  
  • Every blackhole has an escape velocity.  (see Argument 0316)  
  • A blackhole is either overstable, stable, or understable.  (see Argument 0317)  
  • The degree of a blackhole's overstability or undestability changes commensurately with any change in its vergence velocity and/or escape velocity.
  • Blackholes are solidbonded, liquidbonded, or gasbonded depending on the stability condition of their adjacent teelpairs.  (see Argument 0319)  
  • Blackholes of sufficient mass stratify their teelpairs according to their energy measure into a central solidbonded teelcore, surrounded by a liquidbonded teelocean, surrounded by a gasbonded teelosphere.  (see Argument 0320)    

COMMENTARY


In the extremal blackhole concept, for a given spinrate there is a mass measure below which a blackhole cannot endure. This is true, viz:
  • Relative to something, the solidbonded teelcore of a blackhole always spins (rotates).
  • The teelocean and/or teelosphere of a blackhole may spin sympathetically with the teelcore or may be chaotic to a greater or lesser degree. 
  • The spinrate of a blackhole conditions both its vergence and its escape velocity in a multiprocess. 
    • An increase in spinrate triggers a commensurate increase in vergence velocity (because the realspeed of the blackhole's teels has increased).
    • An increase in spinrate triggers a commensurate decrease in escape velocity (because the density of the teels in the blackhole has decreased). 
    • A decrease in spinrate affects the vergence velocity and the escape velocity conversely.
  • In a stable blackhole, an increase in spinrate will be accompanied by a decrease in mass. 
  • In a stable blackhole, a decrease in spinrate will be accompanied by an increase in mass, subject to the availability of teels from beyond the blackhole's gravitysheath interface.
  • In an overstable blackhole, an increase in spinrate will not trigger an alteration in mass until the blackhole becomes understable. 
  • In an overstable blackhole, a decrease in spinrate will be accompanied by an increase in mass, subject to the availability of teels from beyond the blackhole's gravitysheath interface.
  • In an understable blackhole, an increase in spinrate will commensurately increase the rate at which the mass is already decreasing. 
  • In an understable blackhole, a decrease in spinrate will commensurately decrease the rate at which the mass is already decreasing.   








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

Copyright 2013 Peter (Ed) Winchester



REVISIONS

27 May 2014 - Page revised to 3-section format.