THE MALTA COSMOLOGY TEMPLATE



Chapter 07 - Electrons






PARTS

Part 0700
Electrons
Home


Part 0701
Blackholepair

Physics


Part 0702
Blackholepair

Mechanics

Part 0703
Electron

Physics


Part 0704
Electron
Mechanics

Electron
Selfproofs




















Part 0702 - Blackholepair Mechanics

ARGUMENT 0702-06

PRECEDENTS
PARAMETERS
  • Consider an adjacent blackholepair.
  • Consider the blackholes to be "Blackhole A" and "Blackhole B".
  • Consider that each blackhole in the pair is understable.
  • Consider that each blackhole in the pair is centrifugally structured. 
  • Consider that each blackhole gravitonosphere has an "east equator", a "west equator", a "northpole", and a "southpole".
  • Consider that centrifugal gravitonstreams rise at the equator and fall at the poles.
  • Consider that the blackholes are held together by their mutual gravitypull and held apart by their mutual rejectivity and thus subject to the strong force.
  • Consider that the blackholes are so close together that each gravitonosphere intrudes markedly into the other.
REASONING
  • Because the blackholes are held close together, their gravitonosphere gravitonstreams are disrupted. 
  • Because the gravitonstreams are disrupted, the blackholes tumble about each other.
  • In the course of tumbling about each other, the blackholes find and adopt the position of least distress.
    • The position of least distress has the east equator of Blackhole B locked to the southpole of Blackhole A. . 
  • Because the blackholes are in the position of least distress, gravitons stream directly from the east equator of Blackhole B into the southpole of Blackhole A. 
  • Because gravitons are streaming directly into the southpole of Blackhole A, a high gravitonpressure area builds up between the blackhole's southpole and its equator.
  • Because of the high gravitonpressure between the southpole and the equator of Blackhole A, the equatorial upwelling is forced to the blackhole's northpole.
  • Because the equatorial upwelling is now at the northpole, the polar downwelling is overcome. 
  • Because the polar downwelling is overcome, the high level gravitonstreams of Blackhole A now flow from the northpole to the southpole.
  • Because the high level gravitonstreams now flow from the northpole to the southpole, the low level gravitonstreams now flow from the southpole to the northpole. 
  • Thus Blackhole A is now axially structured. 
  • Thus the blackholepair now consists of one centrifugal and one axial blackhole.  
CONCLUSION
  • That countering the blackholepair's mutual gravitypull with its mutual rejectivity results in one blackhole adopting an axial structure.


COMMENTARY 

For a pair of blackholes to be close enough, long enough, for the strong force to kick in requires their vergence velocity to be substantially lower than their escape velocity. In practice, such conditions are only achievable consistently and regularly if a blackholepair is "born" from a single womb. Such wombs did, and do, exist. The first was in the early Universe when blackholes formed in such a density that, notwithstanding their very high kineticenergy, they could bond helically and remain bonded until they had lost enough of their speed. Today's wombs are the stabilisation "throats" of nucleons and atoms which, when engorged, are able to create blackholes of the right size in suitable numbers.







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

Copyright 2013 Peter (Ed) Winchester



HISTORY

19 Nov 2016 - page created.
23 Apr 2017 - changed teels to gravitons.