Astronomy: The Science of the Heavenly BodiesTodd, David P. (David Peck)
History
Astronomy: The Science of the Heavenly Bodies
Todd, David P. (David Peck)
Astronomy
[Illustration: THE 150-FT. TOWER AT THE MT. WILSON SOLAR
OBSERVATORY. At the left is a diagram of tower, telescope
and pit. At the upper right is an exterior view of the
tower; below a view looking down into the pit, 75 ft. deep.
(_Photo, Mt. Wilson Solar Observatory._)]
The focal lengths of object glass and eyepiece will determine just what
distance apart the lenses must be in order to give perfect vision. But
it is quite as important that the axes of all the lenses be adjusted
into one and the same straight line, and then held there rigidly and
permanently. Otherwise vision with the telescope will be very imperfect
and wholly unsatisfactory. The distance from the objective, or object
glass to its focal point is called its focal length; and if we divide
this by the focal length of the eyepiece, we shall have the magnifying
power of the telescope. The eyepiece will usually be made of two lenses,
or more, and we use its focal length considered as a single lens, in
getting the magnifying power. A telescope will generally have many
eyepieces of different focal lengths, so that it will have a
corresponding range of magnifying powers. The lowest magnifying power
will be not less than four or five diameters for each inch of aperture
of the objective; otherwise the eye will fail to receive all the light
which falls upon the glass. A 4-inch telescope will therefore have no
eyepiece with a lower magnifying power than about 20 diameters. The
highest magnifying power advantageous for a glass of this size will be
about 250 to 300, the working rule being about 70 diameters to each inch
of aperture, although the theoretical limit is regarded as 100.
The reason for a variety of eyepieces with different magnifying powers
soon becomes apparent on using the telescope. Comets and nebulæ call for
very low powers, while double stars and the planetary surfaces require
the higher powers, provided the state of the atmosphere at the moment
will allow it. If there is much quivering and unsteadiness, nothing is
gained by trying the higher powers, because all the waves of
unsteadiness are magnified also in the same proportion, and sharpness of
vision, or fine definition, or "good seeing," as it is called, becomes
impossible. The vibrations and tremors of the atmosphere are the
greatest of all obstacles to astronomical observation, and the search is
always in order for regions of the world, in deserts or on high
mountains, where the quietest atmosphere is to be found.
Public-domain text, read in full here on John Shaqi.
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