From the Earth to the moon; and, round the moonVerne, Jules
Science
From the Earth to the moon; and, round the moon
Verne, Jules
Manned space flight -- Fiction; Moon -- Fiction; Science fiction; Space flight to the moon -- Fiction; Space ships -- Fiction
They breakfasted then at two in the morning; the hour mattered little.
Michel served his usual repast, crowned by a glorious bottle drawn from
his private cellar. If ideas did not crowd on their brains, we must
despair of the Chambertin of 1853. The repast finished, observation
began again. Around the projectile, at an invariable distance, were the
objects which had been thrown out. Evidently, in its translatory motion
round the moon, it had not passed through any atmosphere, for the
specific weight of these different objects would have checked their
relative speed.
On the side of the terrestrial sphere nothing was to be seen. The earth
was but a day old, having been new the night before at twelve; and two
days must elapse before its crescent, freed from the solar rays, would
serve as a clock to the Selenites, as in its rotary movement each of
its points after twenty-four hours repasses the same lunar meridian.
On the moon’s side the sight was different; the orb shone in all her
splendor amid innumerable constellations, whose purity could not be
troubled by her rays. On the disc, the plains were already returning to
the dark tint which is seen from the earth. The other part of the
nimbus remained brilliant, and in the midst of this general brilliancy
Tycho shone prominently like a sun.
Barbicane had no means of estimating the projectile’s speed, but
reasoning showed that it must uniformly decrease, according to the laws
of mechanical reasoning. Having admitted that the projectile was
describing an orbit around the moon, this orbit must necessarily be
elliptical; science proves that it must be so. No motive body
circulating round an attracting body fails in this law. Every orbit
described in space is elliptical. And why should the projectile of the
Gun Club escape this natural arrangement? In elliptical orbits, the
attracting body always occupies one of the foci; so that at one moment
the satellite is nearer, and at another farther from the orb around
which it gravitates. When the earth is nearest the sun she is in her
perihelion; and in her aphelion at the farthest point. Speaking of the
moon, she is nearest to the earth in her perigee, and farthest from it
in her apogee. To use analogous expressions, with which the
astronomers’ language is enriched, if the projectile remains as a
satellite of the moon, we must say that it is in its “aposelene” at its
farthest point, and in its “periselene” at its nearest. In the latter
case, the projectile would attain its maximum of speed; and in the
former its minimum. It was evidently moving toward its aposelenitical
point; and Barbicane had reason to think that its speed would decrease
up to this point, and then increase by degrees as it neared the moon.
This speed would even become _nil_, if this point joined that of equal
attraction. Barbicane studied the consequences of these different
situations, and thinking what inference he could draw from them, when
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