Page 291 - The Final Appeal to Mankind

«The Final Appeal to Mankind» by Nicolai Levashov

3,00017 < λb < 3,02037323,

where Δλ may, initially, fluctuate within a range of

0 < Δλ < 0,020203236...

Gradually the secondary deformation of the macrospace dimension (due to the star's
density) becomes even further pronounced, causing the macrospace dimension to
approximate the value of λ7. As this proceeds, the channel between the λ8 and λ7 space-
universe diminishes. The flow of matter from λ7 becomes progressively less.

Concomitantly the star's radiation activity keeps waning until it ceases altogether. This
marks the death of the star. It grows dimmer and dimmer and finally fades away...

(see F Fi ig g. . 1 15 58 8, 1 15 59 9).

By contrast, a star may start out with a huge mass (sixfold that of the sun); then, as it
wanes, it may trigger a secondary deformation of it macrospace dimension, causing it
to dip below the value of λ7:

Δλ ≈ 0.0102018...

Λ6 < λd < λ7; λd = λa - Δλ

The result is an opposite deflection, and a so-called neutron star is born (see F Fi ig g. . 1 15 58 8).

If, initially, the star had a mass greater than tenfold the mass of the sun, the secondary
deformation becomes so great as to establish the linkage between space-universes λ7
and λ6 (see F Fi ig g. . 1 15 59 9).

When this occurs, matter from λ7 starts flowing over to λ6, resulting in the formation
of a black hole. Thus, black holes emerge in the course of the evolution of stars.

Now let us consider how planetary systems are formed.

At the onset of its life span, a star shows a balance between its size, the channel
connecting λ8 and λ7, and the amount of substance flowing through it from space-
universe λ8 (see F Fi ig g. . 1 16 60 0).

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