APPENDIX A
Application to the Home Universe

If a Universe is formed from a near inexhaustible supply of celestial material, then at the 3au criterion (2.7) will still apply, but, also au can be expressed as

au = s"u

3
(A.1)
where now
s"u is the radius of the Universe at the 3au criterion.
Substitution of (A.1) into (2.7) yields after minor reduction
r"u = c2

4pgs"u2
(A.2)
where
r"u is the average density of the Universe with a boundary radius of s"u .

In [3] au for the home Universe was estimated at 4.47 x 1027 cms. From (A.1), using this figure s"u works out to be 13.41 x 1027 cms. Substitution of this figure into (A.2) then gives for r"u the figure of 5.97 x 10-30 gms/cm3.

Now, using the above figures for r"u and s"u in the standard formula for the mass of the Universe gives mu = 6.03 x 1055 gms. This value is the same as that estimated in [3] from a consideration of factors associated with the cosmological time of applicability of modern observations, i.e. tc = 9 billion years from the point of inflexion. In view of this comparative agreement, the consequence is that the home Universe was formed from a near inexhaustible supply of celestial material in the greater Cosmos.

The value of r"u , the average density of the Universe at the 3au criterion, is seen to be some 3 1/ 2 times smaller than that estimated in [3] at tc. Comparative radii and average densities are summarised in the following table.

Point of Measurement PhaseRadiusAverage Density
3au Criterionsu = 3au I ® II13.4E275.97E-30
Point of Inflexionsu = au II4.47E271.6E-28
Cosmological Time of Modern Observationtc II8.7E272.1E-29
Table A1 - Radius/Average Density Comparison for the Home Universe.

Table A1 shows that the expansion of the home Universe at tc in Phase II has only reached some 50% of the distance to the point where su = 3au .

C3 Version 1.0.1
Ó P.G.Bass, March 2006

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