“The western Sun withdraws: meanwhile the Moon,
Full orb’d, and breaking through the scatter’d clouds,
Shows her broad visage in the crimson’d east.”
Early in autumn, when the evenings are frequently clear, many persons
are led with more force than usual to evince an interest in our
satellite, and to desire information which may not be conveniently
obtained at the time. The aspect of the Moon at her rising, near the
time of the full, during the months of August, September, and October,
is more conspicuously noticeable than at any other season of the year,
on account of the position she then assumes on successive nights,
enabling her to rise at closely identical times for several evenings
together. The appearance of her large, ruddy globe at near the same
hour, and her increasing brilliancy as her horizontal rays give way
under a more vertical position, originated the title of “Harvest Moon,”
to commemorate the facility afforded by her light for the ingathering
of the corn preceding the time of the autumnal equinox.
It will be universally admitted that the Moon possesses special
attractions for us, as being situated nearer than any other celestial
body, and forming the inseparable companion or tributary world to the
Earth. The many important influences she exercises have led to her
becoming the object of close investigation; so that her motions and
physical appearances have been ascertained with a remarkable degree
of exactness and amplitude. Her movements regulate the tides; her
positions are of the utmost moment to the mariner; her light is the
welcome beacon of the wayfarer, and its picturesque serenity has ever
formed the theme of poets. To the practical astronomer she constitutes
an orb perfectly unique as regards extent and variety of detail; and
questions relating to the physical condition of her surface, now and in
past ages, supply a fund of endless speculation to the theorist.
The mean apparent diameter of the Moon is 31′ 5″, and it varies from
29′ 21″ at perigee to 33′ 31″ at apogee. Her real diameter is 2160
miles, and her mean distance slightly exceeds 237,000 miles. Her
revolution round the Earth (= sidereal period) is performed in 27^d 7^h
43^m 11^s·46, but the time from one new moon to another (= synodical
period) is 29^d 12^h 44^m 3^s. The Moon’s motion through the firmament
is at the rate of 13° 10′ 35″ per day and 32′ 56″ per hour. Thus she
travels over a space slightly exceeding her own diameter in one hour.
The linear value of 1″ at the distance of our satellite is 1·16 mile,
and of 1′ 69½ miles.
Public-domain text, read in full here on John Shaqi.
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