Everything about Catadioptric System totally explained
A
catadioptric optical system is one which contains both
lenses and
mirrors. Catadioptric systems are commonly used in
telescopes and in lightweight, long focal length
lenses for cameras.
Catadioptric telescopes
Catadioptric telescopes are designs that combine specifically shaped mirrors and lenses to allow very fast
focal ratios (when used at the prime focus), while controlling
coma and
astigmatism.
Telescope makers also use catadioptric designs for any or all of the following reasons:
- They employ spherical surfaces that are easier to manufacture.
- When used in a cassegrain configuration it results in a long focal length instrument that's "folded" into a much smaller package.
- Catadioptric designs are low maintenance and rugged since some or all of their elements are fixed in alignment (collimation).
- Combining a moving primary mirror with a cassegrain configuration allow for large movements in the focal plane to accommodate cameras and CCDs.
- The corrector plates seal the tube assembly from dust and dirt. They also block air currents from the interior of the tube, thereby increasing image stability.
A disadvantage to this design is that the secondary mirror blocks a portion of the light entering the tube.
Schmidt
This design is seen in instruments such as the
Schmidt camera and the
Schmidt-Cassegrain. The first
optical element is a
Schmidt corrector plate. The plate is figured by placing a vacuum on one side, and grinding the exact correction required to correct the
spherical aberration caused by the primary mirror.
Thousands of amateur astronomers have purchased and used Schmidt-Cassegrain telescopes, with diameters from 20 cm (8 in.) to 40 cm (16 in.), since this type of telescope was introduced by
Celestron in the 1960s. Now many companies mass-produce this type of telescope, at prices that make them quite affordable for many amateurs.
Maksutov
The
Maksutov design was invented by
Dmitri Maksutov. It uses an optically transparent "meniscus corrector shell" that's a section of a hollow sphere. It has a spherical primary mirror, and, in the cassegrain configuration, uses a spherical secondary that's often just a mirrored section of the corrector lens. Maksutov-cassegrains tend to have a narrower field of view than Schmidt-Cassegrains due to their longer focal length and are generally heavier as well. However, their small secondary mirror gives them better resolution than a Schmidt-Cassegrain.
Photographic catadioptric lenses
Photographic catadioptric lenses are similar to astronomical catadioptric designs and are used for some of the same reasons (with added modifications to accommodate photographic use). In order to make catadioptric "mirror lenses" less susceptible to blurring from internal air currents caused by external differential heating the internal space is sometimes filled with glass (referred to as a "solid-cat"). The refractive surfaces of the glass combined with added reflective (mirror) coatings are shaped to contribute to the optical properties of the whole mirror assembly, and so such devices are catadioptric. This has the added advantage of making them extremely rugged.
500mm catadioptric lenses are far lighter than a normal 500mm lens, but typically lack an adjustable
diaphragm and operate at a high fixed
f-number equal to the focal ratio of the total optical system. Mirror lenses produce a "doughnut"
bokeh that's generally considered unpleasant. Mirrors don't suffer from
chromatic aberration, thus mirror lenses don't require focus adjustment when used for
infrared photography.
As of 2007, the only catadioptric lens capable of autofocusing is the
Minolta AF 500mm Reflex lens.
Further Information
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