Outlines of a mechanical theory of storms : $b containing the true law of lunar influence, with practical instructions to the navigator, to enable him approximately to calculate the coming changes of the wind and weather, for any given day, and for any part of the oceanBassnett, Thomas
Science
Outlines of a mechanical theory of storms : $b containing the true law of lunar influence, with practical instructions to the navigator, to enable him approximately to calculate the coming changes of the wind and weather, for any given day, and for any part of the ocean
Bassnett, Thomas
Weather
This fraction is, however, too small, as the ablatitious action of the
sun diminishes the attraction of the earth on the moon, in the ratio of
178 29/40 to 177 29/40. So that we must increase the fall of the moon
in the ratio of 711 to 715, and hence the true fall of the moon from the
tangent of her orbit becomes 0.00451 feet per second.
We have found the fall of a body at the surface of the earth, considered
as a sphere, 16.1067 feet per second, and the force of gravity
diminishes as the squares of the distances increases. The polar diameter
of the earth is set down as 7899.170 miles, and the equatorial diameter
7925.648 miles; therefore, the mean diameter is 7916.189 miles.[36] So
that, reckoning in mean radii of the earth, the moon's distance is
59.787925, which squared, is equal to 3574.595975805625. At one mean
radius distance, that is, at the surface, the force of gravity, or fall
per second, is as above, 16.1067 feet. Divide this by the square of the
distance, it is 16.1067/3574.595975805625 = 0.0045058 feet for the force
of gravity at the moon. But, from the preceding calculation, it appears,
that the moon only falls 0.0044510 feet in a second, showing a
deficiency of 1/82d part of the principal force that retains the moon in
her orbit, being more than double the whole disturbing power of the sun,
which is only 1/178th of the earth's gravity at the moon; yet, on this
1/178th depends the revolution of the lunar apogee and nodes, and all
those variations which clothe the lunar theory with such formidable
difficulties. The moon's mass cannot be less than 1/80, and if we
consider it greater, as it no doubt is, the results obtained will be
still more discrepant. Much of this discrepancy is owing to the
expulsive power of the radial stream of the terral vortex; yet, it may
be suspected that the effect is too great to be attributed to this, and,
for this reason, we have suggested that the fused matter of the moon's
centre may not gravitate with the same force as the exterior parts, and
thus contribute to increase the discrepancy.
As there must be a similar effect produced by the radial stream of every
vortex, the masses of all the planets will appear too small, as derived
from their gravitating force; and the inertia of the sun will also be
greater than his apparent mass; and if, in addition to this, there be a
portion of these masses latent, we shall have an ample explanation of
the connection between the planetary densities and distances. We must
therefore inquire what is the particular law of force which governs the
radial stream of the solar vortex. It will be necessary to enter into
this question a little more in detail than our limits will justify; but
it is the resisting influence of the ether, and its consequences, which
will appear to present a vulnerable point in the present theory, and to
be incompatible with the perfection of astronomical science.
LAW OF DENSITY IN SOLAR VORTEX.
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Elsewhere in the archive
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account