Since the gravitation force varies
proportionally to the gravitation constant, it must, according to
the CTH, at the Planck time have been larger than today by the factor
(t1/tPL)
2/3 = (4.7 . 10 17
/ 5.4 . 10 – 44)2/3
» 10 41 i. e.,
it was identical with the strong nuclear force at that time, as demanded
by the Super string theory.
This surprising result even
gains in fascination if we link the strength of both these forces
to their respective range of action.
Fig. 8: Strength and range of action
of fundamental natural forces
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