THE MALTA COSMOLOGY TEMPLATE

Chapter 5 - Darkmatter 

PARTS

Part 2 - Axial Blackholes (cont)

ARGUMENT 0513

• ARGUMENT 0512: 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.

• If the speed and density of a teelstream is beyond that which makes the blackhole semiaxial, it forces the teelospheric equator to the teelospheric southpole. This is an axial blackhole. In an axial blackhole:
  
  
  • Teels are absorbed from the teelstream through which the blackhole is moving in the northern teelospheric hemisphere with the principal absorption point being the teelospheric northpole.
  • Teelstreams within the blackhole's teelosphere move at low level from the northpole to the southpole. At the southpole they rise to move at high level back to the northpole. At the northpole they fall to move at low level to the southpole. And so on.
  • Any excess teels are ejected into the teelstream through which the blackhole is moving from the southern teelospheric hemisphere with the principal ejection point being the teelospheric southpole.

• When the speed and density of a teelstream is even more dominant, it forces the teelospheric equator to the teelospheric southpole and makes the blackhole axial.

• axial blackhole:    The teelosphere of an axial blackhole responds to the spin of the blackhole's teelcore, and to the influence of the teelstream through which the blackhole is moving, by rising at the southpole, moving to the northpole at high level, sinking at the north, proceeding to the southpole at low level, and so on. (see also 'centrifugal blackhole')