The story of the universe. Volume 1 (of 4) : $b The starry skies — John Shaqi
The story of the universe. Volume 1 (of 4) : $b The starry skies
History
The story of the universe. Volume 1 (of 4) : $b The starry skies
Astronomy; Earth (Planet); Natural history
distance separating the middle star of the Bear’s tail from its close
companion.
But this fact of itself is most strikingly suggestive of the vast
distance of the stars. For consider what it means. Imagine the
middle star of the Bear’s tail to be the really nearest of all the
stars instead of lying probably twenty or thirty times further away.
Conceive a comet belonging to that sun after making its nearest
approach to it to travel away upon an orbit requiring 3,000 years
for each circuit. _Then_ (supposing that star equal to our sun in
mass) the comet, though rushing away from its sun with inconceivable
velocity during 1,500 years, would, at the end of that vast
period, seem to be no further away than one-fourth of the distance
separating the sun from its near companion. Look at the middle star
of the Bear’s tail on any clear night, and on its small satellite,
remembering this fact, and the awful immensity of the star-depths
are strongly impressed upon the mind. But the observer must not fail
to remember that the star really is many times more remote than we
have here for a moment supposed, and that such a comet’s range of
travel would be proportionately reduced. Moreover, many among the
stars are doubtless hundreds, even thousands, of times still further
away.
Let us turn lastly to the amazing comet of the year 1744. We find
that though it had the longest period of any which has ever been
assigned to a comet as the result of actual mathematical calculation,
yet its range in space would scarcely suffice to change the
position of the stars in such sort that the aspect of the familiar
constellations would be materially altered. Euler, the eminent
mathematician, calculated for this comet a period of 122,683 years,
which would correspond, I find, to a distance of recession equal to
2,469 times the distance of the earth from the sun, or about eighty
times the distance of Neptune. Yet this is but little more than
twelve times the greatest distance of the comet of 1811. Probably
the actual range of such an orbit from the middle star of the Bear’s
tail would be equal in appearance to the range described above on
the supposition that the star is no further from us than the nearest
known star (Alpha Centauri). That is, such a comet, if it could be
seen and watched during a period of about 122,000 years, would seem
to recede from the star to a distance equal to about one-fourth the
space separating it from its close companion, and then to return to
the point of nearest approach to its ruling sun.
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