Astronomy Explained Upon Sir Isaac Newton's Principles: And made easy to those who have not studied mathematicsFerguson, James
Science
Astronomy Explained Upon Sir Isaac Newton's Principles: And made easy to those who have not studied mathematics
Ferguson, James
Astronomy -- Early works to 1800
In this Construction it is supposed that the Equator, Tropics, Parallel
of _London_, and Meridians through every 15th degree of Longitude are
projected in visible Lines on the Earth’s Disc, as seen from the Sun at
almost an infinite distance; that the Angle under which the Moon’s
diameter is seen, during the time of the Eclipse, continues invariably
the same; that the Moon’s motion is uniform, and her Path rectilineal,
for that time. But all these suppositions do not exactly agree with the
truth; and therefore, supposing the Elements § 367, given by the Tables
to be perfectly accurate, yet the time and phases of the Eclipse deduced
from it’s Construction will not answer exactly to what passeth in the
Heavens; but may be two or three minutes wrong though done with the
utmost care. Moreover, the Paths of all Places of considerable Latitude
go nearer the center of the Disc as seen from the Moon than these
Constructions make them; because the Earth’s Disc is projected as if the
Earth were a perfect sphere, although it is known to be a spheroid.
Consequently, the Moon’s shadow will go farther North in places of
northern Latitude, and farther South in places of southern Latitude than
these projections answer to. Hence we may venture to predict that this
Eclipse will be more annular at _London_ (that is, the annulus will be
somewhat broader on the southern Limb of the Sun) than the Diagram shews
it.
383. Having shewn how to compute the times and project the phases of a
Solar Eclipse, we now proceed to those of the Lunar. And it has been
already mentioned § 317, that when the Full Moon is within 12 degrees of
either of her Nodes, she must be eclipsed. We shall now enquire whether
or no the Moon will be eclipsed _May 18, 1761, N. S._ at 32 minutes past
10 at Night. See page 193.
[Sidenote: Table IV.
Table VI.]
s ° ʹ
Sun from Node at Full Moon in _March 1761_ 9 25 27
Add his distance for two Lunations, to bring it into _May_ 2 1 20
---------
And his distance at Full Moon in that month is 11 26 47
Subtract this from a Circle, or 12 Signs, and there will remain 3° 13ʹ;
which is all that the Sun wants of coming round to the Ascending Node;
and the Moon being then opposite to the Sun, must be just as near the
Descending Node: consequently, far within the limit of an Eclipse.
384. Knowing then that the Moon will be eclipsed in _May 1761_, we must
find her true distance from the Node at that time, by applying the
proper Equations as taught § 363, and then find her true Latitude as
taught in that article.
[Sidenote: Table IV.
Table XIII.
Table XII.]
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