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
But it may be asked: If there be a modifying force in astronomy derived
from another source than that of gravitation, why is it that the
elements of the various members of the system derived solely from
gravitation should be so perfect? To this it may be answered, that
although astronomers have endeavored to derive every movement in the
heavens from that great principle, they have but partially succeeded.
Let us not surrender our right of examining Nature to the authority of a
great name, nor call any man master, either in moral or physical
science. It is well known that Kepler's law of the planetary distances
and periods, is a direct consequence of the Newtonian Law of
gravitation, and that the squares of the periodic times ought to be
proportional to the cubes of the mean distances. These times are given
accurately by the planets themselves, by the interval elapsing between
two consecutive passages of the node, and as in the case of the ancient
planets we have observations for more than two thousand years past,
these times are known to the fraction of the second. The determination
of the distances however, depends on the astronomer, and a tyro in the
science might suppose that these distances were actually measured; and
so they are roughly; but the astronomer does not depend on his
instruments, he trusts to _analogy_, and the mathematical perfection of
a law, which in the abstract is true; but which he does not know is
rigidly exact when applied to physical phenomena. From the immense
distance of the planets and the smallness of the earth, man is unable to
command a base line sufficiently long, to make the horizontal parallax a
sensible angle for the more distant planets; and there are difficulties
of no small magnitude to contend with, with those that are the nearest.
In the occasional transit of Venus across the sun, however, he is
presented with a means of measuring on an enlarged scale, from which the
distance of the sun is determined; and by _analogy_ the distance of all
the planets. Even the parallax of the sun itself is only correct, by
supposing that the square of the periodic time of Venus is in the same
proportion to the square of the periodic time of the earth as the cube
of her distance is to the cube of the earth's distance. Our next nearest
planet is Mars, and observations on this planet at its opposition to the
sun, invariably give a larger parallax for the sun--Venus giving 8.5776″
while Mars gives about 10″. It is true that the first is obtained under
more favorable circumstances; but this does not prove the last to be
incorrect. It is well known that the British Nautical Almanac contains a
list of stars lying in the path of the planet Mars about opposition,
(for the very purpose of obtaining a correct parallax,) that minute
differences of declination may be detected by simultaneous observations
in places having great differences of latitude. Yet strange to say, the
Public-domain text, read in full here on John Shaqi.
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