"Apropos of A. E. Caswell's
suggested law, namely, "the mean distances of the planets from the
sun are proportional to the squares of simple integral numbers," the
writer wishes to point out the following corrections, extensions and other
new laws.
(1) The percentage deviation
from proportionality to the squares of the integers is double that
indicated by him.
(2) Since the earth's distance
is taken as a standard in all measurements, one would expect a good reason
for not assuming its distance to correspond to a perfect square of an integer
(in this case 5). If this is
done the deviations from the above law are as high as 12 per cent.
(3) One would expect similar relations
to hold for the satellites of the planets. For the satellites of Mars the
ratio 52 : 82 holds quite closely.
For the four satellites of Uranus the ratio 52 : 62
: 82 : 92 holds poorly. But for the
satellites of Saturn and Jupiter one must either omit several or resort
to initial numbers greater than 52 for the nearest satellite.
Of course, if large integers are to be admitted one may get as close a
fit as one pleases for almost any distribution of distances. On the whole
the evidence from this source is unfavourable to a deep-seated significance
for the relation cited.
(4) The writer would point
out a relation that depends strictly on the square root of the distance
of a planet from the sun or a satellite from its planet. It is the velocity,
which varies inversely as the square root of the distance from the axis
of revolution. For the planetary system one could then state as a law.
The velocities of the planets are inversely in proportion to simple
integral numbers. Thus:
PLANETS | Period | Velocity | 30.3/Velocity | Integer |
Mercury | 0.2408 | 10.1006 | 3 | 3 |
Venus | 0.6152 | 7.3872 | 4.1 | 4 |
Earth | 1.000 | 6.2832 | 4.83 | 5 |
Mars | 1.88 | 5.0924 | 5.95 | 6 |
Jupiter | 11.86 | 2.7563 | 11.0 | 11 |
Saturn | 29.46 | 2.0344 | 14.9 | 15 |
Uranus | 84.01 | 1.4346 | 21.1 | 21 |
Neptune | 164.6 | 1.1464 | 26.5 | 27 |
(5) Another law may be stated,
as a consequence of Kepler's third law and the distance relation, namely,
the periods of the planets are proportional to the cubes of simple integral
numbers. The same integers as above are involved.
(6) In this connection the
writer would bring to the attention of American scientists an effort by
Viktor Goldschmit to elucidate some of the numerical regularities in the
distances of the planets and satellites from their axes of revolution.
The journal in which it occurs is not generally known. He observes the
distances of the planets to be closely in the sequence 1/13, 1/7, 1/5,
1/3, 1, 2, 4, 6. The four larger planets are considered to have condensed
together before the group of the four smaller ones. A mathematical treatment
strictly analogous to the phenomena of standing waves in sound,
the distribution of lines of spectra, the progress of crystallization and
similar phenomena gives the same law of harmonic relations of distances
not only for the planets but also for satellites. The harmonic sequences
are as follows:
Condensations | 0 | 1/3 | 1/2 | 2/3 | 1 | 3/2 | 2 | 3 |
Large Planets | 0 | -- | 1/2 | -- | 1 | -- | 2 | 3 |
Small planets | 0 | 1/3 | -- | 2/3 | 1 | -- | 2 | -- |
Jupiter's Satellites | 0 | -- | 1/2 | 2/3 | 1 | -- | 2 | -- |
Uranus' Satellites | 0 | -- | 1/2 | 2/3 | 1 | 3/2 | -- | -- |
Saturn inner satellites | 0 | -- | 1/2 | 2/3 | 1 | 3/2 | 2 | -- |
Saturn outer satellites | 0 | -- | -- | -- | 1 | (6/5) | -- | 3 |
Earth - Moon | 0 | -- | -- | -- | 1 | -- | -- | -- |
The sequences are brought into line by transformations derived from considerations of the dominance of certain positions, as the 0, 1 and infinity in condensation.
log d = nk, or enk = d
where d is the distance, k is a constant and n is a simple integer. A fairly accurate straight-line plot is obtained by using values of n for the entire series between Mercury and Neptune, 1, 4, 5, 7, 10, 13, 16, 19 and 21. The interval of 3 predominates. The velocity, v, is related to the above by the relation:
log v = k ' - nk/2
where k ' is another constant and n the same simple
integer as above.
It follows also that a similar logarithmic relation exists for
the periods, that is, a small number of geometric means will determine
the periods.
If p stands for the period, then:
log p = 3/2 nk + k"
where k" is still another constant and n
is the same simple integer as above.
Similar relations may be derived
for centripedal force and the like, but enough has been given here to indicate
the underlying principle."
William M. Malisoff, 1929
Source: MYSTERIOUS UNIVERSE: A HANDBOOK OF ASTRONOMICAL
ANOMALIES
Compiled by William R. Corliss, The Sourcebook Project, Glen Arm
1979: 544-546.