The Practical Astronomer: Comprising illustrations of light and colours--practical descriptions of all kinds of telescopes--the use of the equatorial-transit--circular, and other astronomical instruments, a particular account of the Earl of Rosse's large telescopes, and other topics connected with astronomyDick, Thomas
Science
The Practical Astronomer: Comprising illustrations of light and colours--practical descriptions of all kinds of telescopes--the use of the equatorial-transit--circular, and other astronomical instruments, a particular account of the Earl of Rosse's large telescopes, and other topics connected with astronomy
Dick, Thomas
Astronomical instruments; Astronomy; Telescopes
The _apparent magnitude_ of objects denotes their magnitude as they
appear to us, in contradistinction from their real or true magnitude,
and it is measured by the visual angle; for whatever objects are seen
under the same or equal angles _appear_ equal, however different their
real magnitudes. If a half-crown or half-dollar be placed at about 120
yards from the eye, it is just perceptible as a visible point, and its
apparent magnitude, or the angle under which it is seen, is very small.
At the distance of thirty or forty yards, its bulk appears sensibly
increased, and we perceive it to be a round body; at the distance
of six or eight yards, we can see the king or queen’s head engraved
upon it; and at the distance of eight or ten inches from the eye it
will appear so large, that it will seem to cover a large building
placed within the distance of a quarter of a mile, in other words, the
apparent magnitude of the half-crown held at such a distance, will more
than equal that of such a building, in the picture on the retina, owing
to the increase of the optical angle. If we suppose A (fig. 41.) to
represent the apparent size of the half-crown at nine yards distance,
then we say it is seen under the small angle FED. B will represent its
apparent magnitude at 4-1/2 yards distant under the angle HEG, and the
circle C, its apparent magnitude at 3 yards distant, under the large
angle KEI.
[Illustration: _figure 42._]
This may be otherwise illustrated by the following figure. Let AB (fig.
42.) be an object viewed directly by the eye QR. From each extremity A
and B draw the lines AN,BM, intersecting each other in the crystalline
humour in I: then is AIB the optical angle which is the measure of the
apparent magnitude or length of the object AB. From an inspection of
this figure, it will evidently appear that the apparent magnitudes of
objects will vary according to their distances. Thus AB, CD, EF, the
real magnitudes of which are unequal, may be situated at such distances
from the eye, as to have their _apparent_ magnitudes all equal, and
occupying the same space on the retina MN, as here represented. In like
manner, objects of equal magnitude, placed at unequal distances, will
appear unequal. The objects AB and GH which are equal, being situated
at different distances from the eye, GH will appear under the large
angle TIV, or as large as an object TV, situated at the same place as
the object AB, while AB appears under the smaller angle AIB. Therefore
the object GH is _apparently_ greater than the object AB, though it is
only equal to it. Hence it appears that we have no certain standard of
the _true magnitude_ of objects, by our visual perception abstractly
considered, but only of the _proportions_ of magnitude.
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