THE MALTA COSMOLOGY TEMPLATE



Chapter 5 - Darkmatter 






PARTS



Chapter
Home


Part 1
Centrifugal Blackholes


Part 2
Axial Blackholes


Part 3
Teelospheres as Darkmatter


Part 4
Selfproof
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Part 2 - Axial Blackholes (cont)

ARGUMENT 0512

BROUGHT FORWARD
  • ARGUMENT 0511: When the speed and density of a teelstream is sufficiently dominant, it forces the teelospheric equator to be at 90 degrees to the teelospheric northpole.
REASONING:
  • If the speed and density of a teelstream is beyond that which forces the teelospheric equator to be at 90 degrees to the teelospheric northpole, it forces the teelospheric equator toward the teelospheric southpole.
  • How far it gets toward the teelospheric southpole is commensurate to the additional speed and density of the teelstream.
  • Such a blackhole is no longer fully centrifugal but is not yet fully axial (It is best described as centrifugal with axial characteristics – semiaxial).
CONCLUSION:
  • When the speed and density of a teelstream is even more dominant, it forces the teelospheric equator away from the teelospheric northpole toward the teelospheric southpole to make the blackhole semiaxial.

GLOSSARY:
  • semiaxial blackhole:    A blackhole in which the speed and density of the teelstream through which is moving is enough to move the teelospheric equator toward the teelospheric southpole but not enough to locate it at the teelospheric southpole.
  • teelospheric southpole:    The principal teel ejection point in the teelosphere of an axial blackhole. The teelospheric southpole may or may not coincide with one of the blackhole's teelcore poles.





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Copyright 2013 Peter (Ed) Winchester