OPTICAL DESIGN:
Activities such as astronomy, nature studies and viewing sports must often be done from a distance. For various reasons we cannot get close enough to the subjects to view them in the detail that is needed. Our eyes are general purpose tools and their resolution is limited, their magnifying properties are minimal and they are limited in how much light that they can gather. We must use optical devices such as telescopes to increase our visual range. A telescope is an optical device which makes far objects appear closer. It samples a small area of view, a field, and then magnifies it so that distant objects appear larger. Parallel light rays entering the telescope are
focused to a single point, called the focus or focal point. These focused rays are then magnified with a very powerful lens, or more commonly a set of lenses, called an eyepiece, to give enlarged views of distant objects. The eyepiece acts in the reverse direction to the telescope lens, taking the
focused rays and sending them to the eye as parallel rays. The diameter of the observed circle depends on the field of view of the eyepiece.
Refractors       
Reflectors       
Maksutovs       
REFRACTOR TELECSOPES:
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There are two basic ways to bring light rays to a focal
point. The earliest method used by telescope makers,
was to bend the rays by passing them through one or
more pieces of glass which had curved, polished
surfaces. This method produces a type of telescope
called a refractor.
Refractors have several advantages over other designs.
They are enclosed so that dust and moisture doesn't
enter the optical tube. They have fixed optics so that
they don't require routine collimation, which means
that the optics don't have to be adjusted by the user.
They do not have a central obstruction, which reduces
the amount of light entering the tube and causes an
alteration of the diffraction pattern. The resulting
high-contrast, fine-resolution images produced are
considered ideal for planetary viewing. A problem
with refractors is that since many wavelengths of light
are passing through glass, the uneven bending of the
rays causes false colour, around bright objects. This
must be counteracted with additional lenses and
special glass. Since at least four lens surfaces usually
have to be very accurately shaped, polished and coated,
they are more expensive to produce than other telescope designs.
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REFLECTOR TELECSOPES:
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The second method of focusing light is to reflect the rays off of the surface of a curved mirror, producing a type of telescope called a reflector. The most common reflectors in use today are called Newtonians because this design was pioneered by Isaac Newton.
A mirror is made by coating the front surface of a concave piece of glass with a reflecting material. Light rays entering the telescope reflect off of the mirror and since they never pass through the glass no false colour is produced. The surface of the mirror of a high focal ratio reflector can be shaped or figured to that of the surface of a sphere. This works for small reflectors and those with focal ratios of f/9 or higher. However, with large reflectors and those with focal ratios of f/8 or lower, these spherical mirrors do not bring all of the light rays to the same focal point. The rays from the mirror's perimeter are
focused at a different point from it's centre, resulting in an image which lacks contrast due to spherical aberration.
To overcome this defect, mirror surfaces are shaped during polishing to a paraboloidal shape which
focuses all of the light rays to the same point.
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MAKSUTOV
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Maksutov-Cassegrain telescopes are similar to the Schmidt-Cassegrains. They also have a corrector plate to remove spherical aberration, but they use a thick, meniscus lens instead of a Schmidt lens. Light enters through the concave side of the corrector plate and the primary mirror reflects it back up the tube to the secondary which is often a mirrored spot on the convex side of the corrector plate. As with the Schmidt-Cassegrain, the light rays are reflected through a hole in the primary to reach the eyepiece This design is easier to produce than the Schmidt-Cassegrain, but the thicker corrector plate makes it heavier.
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Telescope Limiting Magnitude
The dimmest star that can be seen without optical aid in a dark sky is around 6
magnitude depending upon the observer's eyesight and sky conditions. Telescope
Limiting Magnitude table gives a rough idea of the faintest star magnitude that
can been seen through a different aperture telescopes. The magnitude values are
not precise because many factors affect the magnitude values such as optics, sky
conditions, etc.
Telescope Limiting Magnitude
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Aperture
Inches |
Aperture
mm |
Faintest
Magnitude |
| 2 |
51 |
10.3 |
| 3 |
76 |
11.2 |
| 4 |
102 |
11.8 |
| 6 |
152 |
12.7 |
| 8 |
203 |
13.3 |
| 10 |
254 |
13.8 |
| 12.5 |
318 |
14.3 |
| 14 |
356 |
14.5 |
| 16 |
406 |
14.8 |
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