16
SURVEY OF THE PROBLEM
the same at all parts of the star. It does not depend on the density nor
on the opacity of the star*. It depends only on the mass and molecular
weight. Moreover, the physical constants employed in the calculation
have all been measured in the laboratory, and no astronomical data are
required. We can imagine a physicist on a cloud-bound planet who has
never heard tell of the stars calculating the ratio of radiation pressure to
gas pressure for a series of globes of gas of various sizes, starting, say, with
a globe of mass 10 gm., then 100 gm., 1000 gm., and so on, so that his
nth globe contains 10 n gm. Table 2 shows the more interesting part of his
results.
Table 2.
No. of Globe
Radiation Pressure
Gas Pressure
30
•00000016
•99999984
31
•000016
•999984
32
•0016
•9984
33
•106
•894
34
•570
•430
35
•850
•150
36
•951
•049
37
•984
•016
38
•9951
•0049
39
•9984
•0016
40
•99951
•00049
The rest of the table would consist mainly of long strings of 9’s and 0’s.
Just for the particular range of mass about the 33rd to 35th globes the
table becomes interesting, and then lapses back into 9’s and 0’s again.
Regarded as a tussle between matter and aether (gas pressure and radia
tion pressure) the contest is overwhelmingly one-sided except between
Nos. 33-35, where we may expect something interesting to happen.
What “happens” is the stars.
We draw aside the veil of cloud beneath which our physicist has been
working and let him look up at the sky. There he will find a thousand
million globes of gas nearly all of mass between his 33rd and 35th globes—
that is to say, between \ and 50 times the sun’s mass. The lightest known
star is about 3 . 10 32 gm. and the heaviest about 2 . 10 35 gm. The majority
are between 10 33 and 10 34 gm. where the serious challenge of radiation
pressure to compete with gas pressure is beginning.
15 . It is remarkable that the units into which the matter of the universe
has aggregated primarily are so nearly alike in mass. The stars differ
* The independence of the opacity seems paradoxical at first, since for given
flow of radiation transparent matter offers less obstruction and experiences less,
force than opaque matter. But this is compensated because the flow of radiation
increases with the transparency of the material.