The Trouvelot astronomical drawings manualTrouvelot, E. L. (Etienne Leopold)
Science
The Trouvelot astronomical drawings manual
Trouvelot, E. L. (Etienne Leopold)
Astronomy -- Pictorial works
diameter, with its system of fractures and its central mountains, which
rise from 3,000 to 4,000 feet above its floor. This crater slopes
southward towards the plain, showing the subsidence to which it has been
submitted. While the northern portion of the wall of this crater rises
to 10,000 feet, that on the plain is only 500 feet high, and is even
wholly demolished at one place where the floor of the crater is in
direct communication with the plain. In the lower part of the _mare_,
and a little to the west of the middle line, is found the crater
Agatharchides, which shows below its north wall the marks of rills
impressed by a flood of lava, which once issued from the side of the
crater. On the left-hand side of the plain, is seen the half-demolished
crater Hippalus, resembling a large bay, which has its interior strewn
with peaks and mountains. On this same side can be seen one of the most
important systems of clefts and fractures visible on the Moon, these
clefts varying in length from 150 to 200 miles.
ECLIPSES OF THE MOON
PLATE VII
Since the Moon is not a self-luminous body, but shines by the light
which it borrows from the Sun, it follows that when the Sun's light is
prevented from reaching its surface, our satellite becomes obscured. The
Earth, like all opaque bodies exposed to sunlight, casts a shadow in
space, the direction of which is always opposite to the Sun's place. The
form of the Earth's shadow is that of a long, sharply-pointed cone,
which has our globe for its base. Its length, varying with the distance
of the Earth from the Sun, is, on an average, 855,000 miles, or 108
times the terrestrial diameter. This conical shadow of the Earth,
divided longitudinally by the plane of the ecliptic, lies half above and
half below that plane, on which the summit of the shadow describes a
whole circumference in the course of a year. If the Moon's orbit were
not inclined to the ecliptic, our satellite would pass at every Full
Moon directly through the Earth's shadow; but, owing to that
inclination, it usually passes above or below the shadow. Twice,
however, during each of its revolutions, it must cross the plane of the
ecliptic, the points of its orbit where this happens being called nodes.
Accordingly, if it is near a node at the time of Full Moon, it will
enter the shadow of the Earth, and become either partly or wholly
obscured, according to the distance of its centre from the plane of the
ecliptic. The partial or total obscuration of the Moon's disk thus
produced constitutes a partial or total eclipse of the Moon. The
essential conditions for an eclipse of the Moon are, therefore, that our
satellite must not only be full, but must also be at or very near one of
its nodes.
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