68. Now in order to explain the reason of the moon's appearing greater
than ordinary in the horizon, it must be observed that the particles
which compose our atmosphere intercept the rays of light proceeding from
any object to the eye; and by how much the greater is the portion of
atmosphere interjacent between the object and the eye, by so much the
more are the rays intercepted; and by consequence the appearance of the
object rendered more faint, every object appearing more vigorous or more
faint in proportion as it sendeth more or fewer rays into the eye. Now
between the eye and the moon, when situated in the horizon, there lies a
far greater quantity of atmosphere than there does when the moon is in
the meridian. Whence it comes to pass that the appearance of the
horizontal moon is fainter, and therefore by sect. 56 it should be
thought bigger in that situation than in the meridian, or in any other
elevation above the horizon.
69. Farther, the air being variously impregnated, sometimes more and
sometimes less, with vapours and exhalations fitted to retund and
intercept the rays of light, it follows that the appearance of the
horizontal moon hath not always an equal faintness, and by consequence
that luminary, though in the very same situation, is at one time judged
greater than at another.
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