(Redirected from Refractor telescope)
Image of a refracting telescope from the Cincinnati Observatory in 1848
A 'refracting' or 'refractor telescope' is a
dioptric telescope that uses a
lens as its
objective to form an image. The refracting telescope design was originally used in
spy glasses and
astronomical telescopes but is also used in other devices such as
binoculars and long or
telephoto camera lenses.
Invention
Main articles: History of telescopes
Refractors were the earliest type of
optical telescope. The first practical refracting telescopes appeared in the
Netherlands about 1608, and were credited to three individuals,
Hans Lippershey and
Zacharias Janssen, spectacle-makers in
Middelburg, and
Jacob Metius of
Alkmaar also known as Jacob Adriaanszoon.
Galileo, happening to be in
Venice in about the month of May 1609, heard of the invention and constructed a much improved version of his own based on his understanding of the effects of refraction. Galileo then communicated the details of his invention to the public, and presented the instrument itself to the
doge Leonardo Donato, sitting in full council. Galileo may thus claim to have invented the refracting telescope independently, but not until he had heard that others had done so.
Refracting telescope designs
A typical refractor has two basic elements, a
convex objective lens and an
eyepiece lens. The objective in a refracting telescope
refracts or bends
light at each end using
lenses. This refraction causes
parallel light rays to converge at a
focal point; while those which were not parallel converge upon a
focal plane. This can enable a user to view the image of a distant object as if it were
brighter,
clearer, and/or
larger. Refracting telescopes can come in many different configurations to correct for image orientation and types of aberration.
Galilean telescope
The original design Galileo came up with is commonly called a 'Galilean telescope'. It uses a convex objective lens and a concave eyepiece lens.
The first telescope used the same principles that all telescopes would rely upon. The combination of the two lenses gathered more light than the human eye could collect on its own, focused it, and formed an image. Because the image was formed by the bending of light, or refraction, these telescopes came to be known as refracting telescopes or, simply, refractors.
Galileo’s best telescope magnified objects about 30 times. Because of flaws in its design, such as the shape of the lens, the images were blurry and distorted. But it was good enough for Galileo to explore the sky.
Keplerian Telescope
The 'Keplerian Telescope', invented by
Johannes Kepler in 1611, is an improvement on Galileo's design. It uses a convex lens as the eyepiece instead of Galileo's concave one. The advantage of this arrangement is the rays of light emerging from the eyepiece are converging. This allows for a much wider field of view and greater eye relief but the image for the viewer is inverted. Considerably higher magnifications can be reached with this design but to overcome aberrations the simple objective lens needs to have a very high
f-ratio (
Johannes Hevelius built one with a 45 m (150 ft)
focal length). The design also allows for use of a
micrometer at the focal plane (used to determining the angular size and/or distance between objects observed).
Achromatic refractors
Main articles: Achromatic telescope
The '
Achromatic' refracting lens was invented in 1733 by an English barrister named
Chester Moore Hall although it was independently invented and patented by
John Dollond. The design limits the effects of
chromatic and
spherical aberration by using an objective made of two pieces of
glass (with different
dispersion), "
crown" and "
flint glass". Each side of each piece is ground and
polished, and then the two pieces are assembled together. Achromatic lenses are corrected to bring two
wavelengths (typically red and blue) into focus in the same plane.
Apochromatic refractors
Main articles: Apochromat
'Apochromatic refractors' have objectives built with special, extra-low dispersion materials. They are designed to bring three wavelengths (typically red, green, and blue) into focus in the same plane. The residual color error (secondary spectrum) can be up to an order of magnitude less than that of an achromatic lens. Such telescopes contain elements of
fluorite or special, extra-low dispersion (ED) glass in the objective and produce a very crisp image that is virtually free of chromatic aberration. Such telescopes are sold in the high-end amateur telescope market. Apochromatic refractors are available with objectives of up to 553 mm in diameter, but most are between 80 and 152 mm.
Technical considerations
Refractors have been criticized for their relatively high-degree of residual
chromatic and
spherical aberration. This affects shorter
focal lengths more than longer ones. A 4" achromatic refractor is likely to show considerable color fringing (generally a purple halo around bright objects). A 4" 16 will have little color fringing.
In very large apertures, there is also a problem of
lens sagging, a result of
gravity deforming
glass. There is a further problem of glass defects, striae or small
air bubbles trapped within the glass. In addition, glass is
opaque to certain
wavelengths, and even
visible light is dimmed by reflection and absorption when it crosses the air-glass interfaces and passes through the glass itself. Most of these problems are avoided or diminished by using reflecting telescopes, that can be made in far larger apertures.
Notable refracting telescopes
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Yerkes Observatory 102 cm
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Swedish Solar Telescope (100cm)
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Lick Observatory (91cm)
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Paris Observatory (83 cm + 62cm)
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Nice Observatory (76cm)
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Archenhold Observatory (68cm, 21 m focal length - the longest refracting telescope ever built)
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Lowell Observatory (24 in)
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Chabot Space & Science Center (20 in, 8 in)
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Griffith Observatory (12 in)
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Dearborn Observatory (18.5 in)
See also
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Reflecting telescopes
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Catadioptric telescopes
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Astrograph
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List of largest optical refracting telescopes, from which it is clear that their heyday was in the 19th century