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Cassegrain telescope

Reflecting telescope
synonym Cassegrain telescope (Cassegrain telescope) Generally refers to Cassegrain telescope
Cassegrain telescope: composed of two reflector Constituent Reflecting telescope It was invented by Cassegrain in 1672. The large one in the mirror is called Primary mirror , small ones are called Secondary mirror Usually in the center of the main mirror Opening , imaged behind the primary mirror. Its focus is called Cassegrain focus. Sometimes, according to the figure Dotted line Add one more slant Plane mirror , imaging on the side, this Cassegrain telescope, also known as Nemesis telescope.
Chinese name
Cassegrain telescope
Foreign name
Cassegrain
reflector
Two pieces
Invention
Cassegrain
Invention time
1672

Invention and design

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Cassegrain telescope
The Cassegrain telescope is designed to Bernhard Schmidt Based on the Schmidt star camera Spherical mirror Make the primary mirror and correct it with the correction plate Spherical aberration Following the design of Cassegrain convex mirror do Secondary mirror , reflect light through Primary mirror The central hole converges behind the primary mirror focal plane On. Some designs add other optical elements near the focal plane, such as a flat field mirror.
The U.S. Celestron Terran C9.25 Cassegrain type telescope has many deformations (double Spherical mirror , Double Aspherical mirror , or spherical mirror and aspherical mirror), which can be divided into two main design forms: compact and non compact.
In a tight design, the correction plate is close to or just in the Primary mirror Focus on; The non compact correction plate is close to or on the main mirror curvature On the center (twice the focal length).
A typical example of tight design is the Celestron and Meade products, which combine a solid primary mirror with a small curvature Large Secondary mirror In this way, although the breadth of vision is sacrificed, the lens tube can be shrunk to a very short length. Most tightly designed Celestron and Meade primary mirrors Coke ratio Is f/2, while the secondary mirror is negative f/5, resulting in a system focal ratio of f/10. The exception to be mentioned is Celestron's C-9.25. The focal ratio of the primary mirror is f/2.3, and the focal ratio of the secondary mirror is f/4.3. As a result, the lens barrel is longer than the general compact model, and the field of vision is relatively flat.
The non compact design makes the correction plate close to or on the curvature center of the primary mirror. A very good example of Schmidt Cassegrain design is concentric, which means that the curvature center of all mirrors is at one point: the curvature center of the primary mirror. Optically, the non compact design can produce better Flat field And modification, but the length of the lens barrel has increased.

Main types

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Cassegrain telescope
⒈Classical Cassegrain paraboloid Hyperboloid
2. Ritchey Chretien hyperboloid bisurface
3. Dall Kirkham ellipsoidal sphere
⒋Houghton-Cassegrain Biconvex lens + Biconcave lens Spherical sphere
5. Any Schmit Cassegrain corrector surface type
6. Maksutov Cassegrain meniscus spherical surface
7. Schmidt meniscus Cassegrain corrector+meniscus lens spherical surface
8. Multiple Mangin Classrain Spherical lens Spherical sphere
9. Pressmann Camichel spherical elliptical surface
© Schiefspiegler oblique reflection off-axis

structural style

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Classical Cassegrain
(Classic Cassegrain system):
Structural characteristics of optical telescope
The "traditional" Cassegrain telescope has Parabolic mirror Of Primary mirror , and Hyperboloid Of Secondary mirror The light is reflected and passed through the hole in the center of the main mirror, and the design of folding optics makes the length of the mirror tube shrink. In the lens of small telescopes and cameras, the secondary mirror is usually installed in the transparent part of the closed telescope tube optical glass On board Optical platform Such device can eliminate the "star shape" caused by spider shaped support frame Scattering effect Although closing the mirror tube will cause Amount of light But the barrel can be kept clean, Primary mirror It can also be protected.
It uses hyperboloid and paraboloid Some characteristics of reflection, concave Of Parabolic reflector You can parallel optic axis All incident rays converge at a single point - focus; Convex surface Of Hyperboloid reflector There are two focal points, which reflect all rays passing through one focal point to the other. The lens of this type of telescope is designed Huian It is placed at a position where the light can share a focus, so that the light can Face mirror Is imaged at the other focus for observation, usually external eyepiece It will also be at this point. The primary mirror of the paraboloid will enter the Directional light Reflect and converge on the focus. This point is also hyperbola A focal point of the mirror. Then the hyperboloid mirror reflects these rays to another focus, where you can observe the image
Ritchey- chretien
(R-C system, Richie Kleikion):
Structural characteristics of optical telescope
Light parallel to the optical axis, satisfaction, etc Optical path Cassegrain telescope with sine condition. It was proposed by H. Chretien R-C telescope Its focus is called R-C focus. The main Secondary mirror Shape is very close to rotation Hyperboloid In practice, this system can be approximately regarded as eliminating three levels Spherical aberration and Coma A system of rotating hyperboloids. Due to the elimination of coma field It is larger than other forms of Cassegrain telescope, and the image spot is symmetric ellipse. If a curved negative is used, the field of view will be significantly increased, and the image spot will be circular. One primary mirror relative aperture 1/3, the relative aperture of the system is 1/8, and the image is not far behind the primary mirror. The eccentricity of the primary mirror is close to the hyperboloid of 1.06, and the secondary mirror Eccentricity Hyperboloid close to 2.56. On the ideal image plane (image plane of paraxial light), if the image spot dispersion is required to be no more than 1, it can be used Field diameter About 19 '; If bending negative film is used, the image spot dispersion is still required to be no more than 1, and the field diameter can reach 37 '. To get a larger field of view, you need to add Image field correction lens join Image field correction Of R-C telescope It is also better than Cassegrain telescope with parabolic primary mirror. But when the main focus is used in the R-C telescope, the image is Spherical aberration Of. Therefore, at least one correction lens or reflector
Typical Cassegrain system Primary mirror Is a paraboloid, Secondary mirror It is hyperboloid, so only spherical aberration can be corrected. If the primary mirror is also changed to hyperboloid, two kinds of correction can be made aberration , spherical aberration sum Coma field It can also be increased appropriately, but it needs to be corrected in order to further increase the field of view Field music Astigmatism And distortion, which requires adding a set of correction lenses composed of at least two lenses in the image side, which can be called Field mirror
Dall-Kirkham cassegrain
(Da Kekaseglin)
Structural characteristics of optical telescope
The Dar Chickham Kaseglin telescope was designed by Hollersdale in 1928 and edited by the then scientific American in 1930 Amateur astronomer Alan Chickham and Albert G. Ingel wrote a paper and published it in the magazine. This design uses concave elliptical mirror as the primary mirror, convex Spherical mirror Do second reflector This system is easier to grind than Cassegrain's or Richie Klein's systems, but there is no correction for off-axis Coma aberration and field Distortion, so the image quality will quickly deteriorate when it leaves the axis. But for the long Coke ratio Since the influence of F/15 is small, the mirror with focal ratio above F/15 will still adopt this form of design.
Houghton -cassegrain
(H-C system, Holden Cassegrain): two spheres reflector
Structural characteristics of optical telescope
Hougton's Corrector By a piece Biconvex lens And a pair Concave mirror Composition, can be well corrected Spherical aberration Coma , distortion, available field Very large, the color difference is also very small and can be ignored aberration Mainly off-axis astigmatism, all surfaces are spherical, Radius of curvature Larger (unlike the small curvature radius of Maksutov's corrector), it is easy to process and has lower requirements for materials In terms of installation, Corrector The distance between the two lenses and the distance between them and the main mirror has a large tolerance, mainly for aligning the optical axis
Hougton performs well both visually and photographically Personally, Hougton is big Coke ratio (Fast) It can better reflect its advantages when used for photography If the focal ratio is small, there is no obvious advantage compared with the parabolic Niu inverted telescope. Some foreign DIYers have made Hougton Niu telescopes It can be said that this type of mirror is the only one DIYER can make In addition, in the oslo It has been tested. When the aperture is small (such as 100mm, 120mm) Biconvex lens Change to convex flat mirror, double Concave mirror Change to concave flat mirror, although some will be introduced aberration , but very small (according to the photographic requirements). As long as the requirements are not quite high, they are completely within the acceptable range. Schmidt Cassegrain type
schmit-cassegrain
Structural characteristics of optical telescope
Schmidt Cassegrain telescope is a kind of Catadioptric telescope The folded light path is combined with the correction plate to form a compact astronomical instrument. Schmidt -Cassegrain's design is based on Bernhard Schmidt Based on Schmidt star camera, just like Schmidt star camera Spherical mirror As the primary mirror Schmidt corrector plate To correct Spherical aberration Following the design of Cassegrain convex mirror do Secondary mirror , reflect the light through the hole in the center of the main mirror, and converge Primary mirror Rear focal plane On. Some designs add other optical elements near the focal plane, such as a flat field mirror.
Schmidt Cassegrain type
It has many deformations (double spherical mirror, double aspherical mirror, or spherical mirror and aspherical mirror each), and can be divided into two main design forms: compact and non compact. In a compact design, the correction plate is close to or at the focus of the primary mirror; The non compact correction plate is close to or just on the curvature center of the primary mirror (twice the distance of the focal length). A typical example of tight design is the Celestron and Meade products, which combine a solid primary mirror with a small curvature Large Secondary mirror In this way, although the breadth of vision is sacrificed, the lens tube can be shrunk to a very short length. Most tightly designed Celestron and Meade primary mirrors Coke ratio Is f/2, while the secondary mirror is negative f/5, resulting in a system focal ratio of f/10. The exception to be mentioned is Celestron's C-9.25. The focal ratio of the primary mirror is f/2.3, and the focal ratio of the secondary mirror is f/4.3. As a result, the lens barrel is longer than the general compact model, and the field of vision is relatively flat. The non compact design makes the correction plate close to or on the curvature center of the primary mirror. A very good example of Schmidt Cassegrain design is concentric, which means that the curvature center of all mirrors is at one point: the curvature center of the primary mirror. Optically, the non compact design can produce better flat field and deformation correction than the compact design, but the length of the barrel is increased.
Maksutov-cassegrain
Maksutov Kaseglin style:
Structural characteristics of optical telescope
Maksutov is a refracting reflecting (mirror lens) telescope designed to reduce off-axis aberration , for example Coma aberration In 1944, Soviet Union Photologist Demetri Maksutov invented this type of telescope Spherical mirror As the primary mirror and combined with incident light Holey Lunate To correct Spherical aberration , this is Reflecting telescope And other types of Major issues The biggest disadvantage of the Maksutov type is that it can not produce large caliber (>250mm/10in), because the weight and production cost will rise due to the inhibition of the correction plate.
Maksutov objective lense Not able to correct the whole beam Spherical aberration , only the edge spherical aberration can be corrected, so there is residual spherical aberration aberration For example, only correction Coma , cannot be corrected Astigmatism At the time of his invention, Marksutov himself suggested that it was possible to replace Cassegrain's "folding" optical structure. Perkin Elmer The designer John Gregory developed the Maksutov Cassegrain telescope from the idea of Maksutov. Later, Gregory Sky and telescope The magazine published the landmark design of the f/15 and f/23 Maksutov Cassegrain telescopes, which clearly foresaw the commercial use of this design for Perkin Elmer.
Optical telescope
Many of the Mark Sutov styles that have been made use of the design of "Kaseglin" (sometimes called "Dot Mark Sutov"), the original Secondary mirror It is replaced by a small piece of aluminum spot on the inside of the correction plate. The advantage is that it has been fixed without alignment and calibration, and it also eliminates the problems caused by spider shaped support frame Diffraction fringe The disadvantage is that a certain degree of freedom (the radius of curvature of the secondary mirror) is lost, because the radius of curvature of the secondary mirror must be consistent with the inside of the meniscus correction plate. Gregory himself, for the second time, Redesign If the speed is fast (f/15), the front of the correction plate or the main mirror is aspheric to reduce the aberration.
Schmidt-meniscus Cassegrain
Schmidt lunate Cassegrain
This type of telescope can be said to combine the advantages of Schmidt and Marksutov, so it is equivalent to calling two kinds of correctors, Schmidt is used for correction Spherical aberration The crescent moon is used to correct the coma, but this type of Cassegrain is too long for large caliber.
Mangin-Cassegrain
Agunov Kaseglin
Structure of Cassegrain Telescope
The Agunov Cassegrain telescope was designed by P P. Agunov was first introduced to the world. All his optics are Spherical mirror And the traditional Cassegrain style Secondary mirror Replace with three lens elements with air gaps. The lens furthest from the main mirror is the Manjing mirror, which functions as the surface of the second mirror, and has a reflective coating on the side facing the sky. Agunov's system only uses spherical surfaces to avoid aspheric surface Manufacturing and testing. However, it seems that the benefits obtained are very few, because this system is actually very difficult to make, and it requires an accurate radius of curvature of the free zone sphere to replace the equivalent aspherical mirror.
Pressmann-Camichel
Presman Carmichael Cassegrain
Optical telescope
Compared with the above types of Cassegrain, the Pressmann Camichel Type is the easiest to manufacture, but its quality is poor. It can only be used with Schmidt corrector.
Schiefspiegler
Off Axis or Oblique Reflection reflector Cassegrain:
Optical telescope
The Schiefspiegler ("off-axis" or "oblique reflection") mirror is a very strange Cassegrain reflector , he will primary mirror Tilt to avoid the second reflector Primary mirror Creates a shadow on the. Although the diffraction pattern is eliminated, it leads to other different aberration It must be corrected.
Three-mirror Cassegrain
Cassegrain
Cassegrain telescope
three reflector The system is composed of three mirrors, with two spacing, three radii and three cone coefficients, totally eight variables. In addition to meeting the system focus Spherical aberration Coma Astigmatism, field curvature, etc system performance In addition to image quality requirements, there are enough variables for system layout and structure optimal design Three mirror system is better than two mirror system field Large and easy to control optical system Stray radiation of the off axis field of view Luminous flux To make the illumination of the image surface more uniform. along with space technology The development of total reflection optical system, especially the three Reflective optical system It is gradually becoming the main form of space optical system.

practical application

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Optical telescope
At Cassegrain telescope Larger ones can be placed at the focus terminal equipment It does not block the light, and the observation operation is convenient. For one with both Main focus system Cassegrain system and folding axis system relative aperture It is medium. It is suitable for medium light intensity and large light intensity scale Generally, the main work carried out here is relatively large a spectrometer Of Spectroscopic Observation, direct photography and image intensifier Photography Photoelectric photometry And infrared observation.
This design is very common on telescopes provided by manufacturers to consumers, because spherical Optical surface Not only is it better than long focal length Refracting telescope Easy to make. Although this kind of telescope is better than Same caliber Of Reflecting telescope The price is more expensive, but because of the compact optical design, it is easy to carry within the designed aperture, making it Astronomer It has become a mainstream amateur high-end astronomical observation instrument. High Coke ratio It means it is different from the former Schmidt The astrograph is not a wide-angle telescope, but its narrow field of view is very suitable for observing planets and deep space [1]