The Mirror of Literature, Amusement, and Instruction - Volume 10, No. 267, August 4, 1827 by Various
page 13 of 49 (26%)
page 13 of 49 (26%)
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appearance, "like a pure flame that shot across the heavens."
Dr. Herschel made many observations on this portion of the heavens, using a Newtonian reflector of twenty feet focal length, and an aperture of eighteen inches. With this powerful telescope he completely resolved the whitish appearance into stars, which the telescopes he had formerly used had not light enough to do. In the most vacant place to be met with in that neighbourhood, he found sixty-three stars; other six fields, or apparent spaces in the heavens, which he could see at once through his telescope, averaged seventy-nine stars in each field: thus he found that by allowing 15 min. of a deg. for the diameter of his field of view, a belt of 15 deg. long, and 2 deg. broad, which he had often seen pass before his telescope in an hour's time could not contain less than 50,000 stars, large enough to be distinctly numbered, besides which he suspected twice as many more, which could be seen only now and then by faint glimpses, for want of sufficient light. In the most crowded part of that region he informs us, he has had fields of view which contained no less than 588 stars, and these were continued for many minutes, so that in one quarter of an hour's time there passed no less than 116,000 stars. He also intimates the probability of the sun being placed in this great stratum, though perhaps not in the very centre of its thickness. From the appearance of the galaxy it seems to encompass the whole heavens, as it certainly must if the sun be within the same. From succeeding observations made by Dr. Herschel, he gathers that the milky way is a most extensive stratum of stars of various sizes, and our sun evidently one of the heavenly bodies belonging to it. In viewing and gauging this shining zone in almost every direction, he found the number of stars composing it, by the account of those gauges constantly increase and decrease in proportion to its apparent brightness to the |
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