THE MALTA COSMOLOGY TEMPLATE



Chapter 03 - Blackholes






PARTS

Part 0300
Blackhole
Home Page


Part 0301
Gravitonpair

Physics

Part 0302
Blackhole

Physics

Part 0303
Blackhole

Structure

Part 0304
Blackhole Mechanics


Part 0305
Blackhole Attunement


Blackhole Selfproofs


















Blackhole Selfproofs

SELFPROOF 0304 - EXTREMAL BLACKHOLE

CURRENT PARADIGM

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

MALTA TEMPLATE

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 gravitoncore of a blackhole always spins (rotates).
  • The gravitonocean and/or gravitonosphere of a blackhole may spin sympathetically with the gravitoncore or may be chaotic to a greater or lesser degree. 
  • The spinrate of a blackhole conditions both its vergence velocity 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 gravitons has increased).
    • An increase in spinrate triggers a commensurate decrease in escape velocity (because the density of the gravitons 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 gravitons 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 gravitons 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.
10 Apr 2015 - Major revisions to layout, content, and numbering.
24 Apr 2016 - Revisions to content.
22 Apr 2017 - change teels to gravitons.