| The Celestial Sphere |
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| The celestial sphere is an imaginary sphere of infinite radius centred on the Earth, on which all celestial bodies are assumed to be projected. This Earth-centred Universe is, of course, not an accurate model of the real Universe, so why introduce it? There are two reasons why the concept of a celestial sphere is useful. First, it forms a convenient pictorial representation of the different directions of astronomical objects, and second, calculations involving these directions can be performed using some formulae of spherical trigonometry. The celestial sphere is illustrated in this figure. The celestial sphere is assumed to be fixed, so as the Earth rotates the celestial sphere appears to rotate in the opposite direction once per day. This apparent rotation of the celestial sphere presents us with an obvious means of defining a coordinate system for the surface of the celestial sphere - the extensions of the north pole (NP) and south pole (SP) of the Earth intersect with the north celestial pole (NCP) and the south celestial pole (SCP), respectively, and the projection of the Earth's equator on the celestial sphere defines the celestial equator (CE). The celestial sphere can then be divided up into a grid in a similar manner to the way in which the Earth is divided up into a grid of latitude and longitude. |
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We can never observe the whole celestial sphere from the Earth as the
horizon limits our view of it. In fact, we can only ever observe half of the celestial
sphere at any one time, the half we observe depending on our position on the Earth's
surface, as shown in figure above. In this figure, the observer has the impression of
being on a flat plane and at the centre of a vast hemisphere across which the celestial
bodies move. On all sides, the plane stretches out to meet the base of this celestial
hemisphere at the horizon. The point directly overhead the observer (as defined
by a line passing through the centre of the Earth and perpendicular to the horizon) is
known as the zenith. The point opposite this, which the observer cannot see, is
known as the nadir. Because the radius of the celestial hemisphere is infinite
compared with the radius of the Earth, the directions of the north celestial pole and
the celestial equator as viewed by the observer (north celestial pole and celestial
equator for an observer) are indistinguishable from their real directions (north celestial
pole and celestial equator for the earth's equator), which are defined relative to the
centre of the Earth. As the observer moves further north in latitude, the north celestial
pole moves closer to the zenith until they become coincident when the observer is at the
north pole. At the north pole, the celestial equator lies on the horizon. As the observer
moves further south in latitude, the north celestial pole moves further away from the
zenith until it lies at the horizon when the observer is at the Earth's equator. At the
Earth's equator, the celestial equator passes through the zenith. The stars are sufficiently distant that for our purposes we can assume that they are fixed to the celestial sphere. This is not true of solar system objects (e.g. the Sun, Moon, planets, comets, asteroids and spacecraft) which move (albeit slowly) with respect to the celestial sphere. We will return to the motion of solar system objects (and, in particular, the Sun) on the celestial sphere in the end of this section. For now, we will concentrate on the motions of the stars. The Earth rotates from west to east and hence the stars appear to revolve from east to west about the celestial poles on circular paths parallel to the celestial equator once per day. Some stars never set and remain visible at night all year. These are called circumpolar stars. A circumpolar star at its maximum elevation above the horizon is said to be at its upper culmination. Similarly, a circumpolar star at its minimum altitude above the horizon is said to be at its lower culmination. Stars further from the pole rise, attain a maximum altitude above the horizon (when they are said to transit) and then set below the horizon. These stars are visible at night only during that part of the year when the Sun is in the opposite part of the sky. |
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| Which stars are circumpolar
depends on the latitude of the observer; stars within an angle between the north
pole and the horizon (the observer's latitude) are circumpolar for an observer at
northern-hemisphere latitude (of the observer), and stars within the same angle but
of the south pole are never seen by such an observer; the reverse is true for an
observer in the southern hemisphere. This means that for observers at the Earth's
poles, all of the stars are circumpolar and the observers never see any of stars in
the opposite hemisphere. For observers at the Earth's equator, none of the stars are
circumpolar and the observers see the whole celestial sphere during the course of a
year. As mentioned above, the Sun not only revolves with the stars on the celestial sphere each day, it also moves much more slowly along a path relative to the stars, making one revolution of this path in one year. This motion is due to the fact that the Earth makes one rotation of the Sun each year and because the Sun is much closer to the Earth than the stars. An observer who notes each month what group of stars is first visible above the western horizon after sunset will notice that there is a regular progression along a strip in the celestial sphere. The constellations along this strip are known as the signs of the zodiac. |
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| The apparent path of the Sun
in the sky is known as the ecliptic and is actually the intersection of the plane
of the Earth's orbit with the celestial sphere. Because the rotation axis of the Earth
(which defines the celestial sphere) is tilted at an angle (23.5°) with respect to
the plane of the Earth's orbit, the ecliptic is inclined at an angle to the celestial
equator, as shown in the figure. The angle is known as the obliquity of the ecliptic
and is currently about 23°27'. The ecliptic and the equator intercept at
two points, associated with the zodiacal constellations of Aries and Libra. The first
point of Aries is defined to be the point where the Sun, moving along the ecliptic,
crosses the celestial equator from south to north. This occurs at the spring equinox
(or vernal equinox), on March 21, when day and night are of equal length
(hence the name). The first point of Aries is sometimes referred to as the vernal (or
spring) equinox and marks the beginning of spring in the northern hemisphere. Day and
night are also of equal length at the autumnal equinox, on September 21, when
the Sun crosses the celestial equator from north to south in the constellation of Libra.
The autumnal equinox marks the beginning of autumn in the northern hemisphere. The maximum altitude of the Sun in the sky, as viewed from the northern hemisphere, gradually increases from the spring equinox until it reaches a maximum on June 21 - the summer solstice (when the Sun appears to `stand still' in the sky before starting to move back towards the celestial equator). At the summer and winter solstices the Sun is directly overhead at noon at the Tropics of Cancer and Capricorn, respectively, these being the zodiacal constellations associated with those parts of the ecliptic where the Sun is at these times. The summer solstice marks the beginning of northern hemisphere summer. Similarly, the Sun reaches its minimum altitude in the sky when viewed from the northern hemisphere on December 21 - the winter solstice - which marks the beginning of northern hemisphere winter. The first point of Aries forms the basis of the most often used celestial coordinate system. |
| How do telescopes work? - Components and Optical Properties | |
| There are two basic types of telescopes. Refractors and reflectors. Both have their advantages. Refracting telescopes gather light with a lens, directing it to the eyepiece. Small starter scopes are often of this type, as they are simple to operate and maintain. Larger refractors, however, become very expensive and are typically bought by avid enthusiasts. Reflecting telescopes gather light with a mirror, reflecting it before directing it to the eyepiece. | |
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Setting up a telescope includes the main scope, a finderscope, more than one eyepiece, a tripod (and perhaps a camera adapter). Aperture is the diameter of the lens or mirror that collects light. The magnification of your telescope is limited by the aperture. A larger aperture collects more light, allowing for greater resolution and higher magnification. The distance light travels inside the telescope is the focal length. The eyepiece, has its own focal length. The power of a telescope, often called magnification, is determined by dividing the focal length of the telescope by the focal length of the eyepiece. A finderscope is crucial to a good setup; it helps you find and center objects that would be elusive in the higher-powered main telescope. The finderscope must be adjustable so that it can be aligned with the main scope. A solid base, either a table-mount or a tripod similar to that used by a camera, is critical to steady viewing. |
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Light Gathering Power A=p(D/2)2 |
The primary function of an astronomical telescope is to collect light. The light gathering power of a telescope is measured by the area of the light collector (either a lens or a mirror). A telescope's size is always specified by the diameter of its primary mirror. The area of a circular primary mirros is given by the equation on the left column. |
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Resolving Power a=4.56/D |
The resolving power if the ability of a telescope to separate two close images or to see fine detail in an image. Greater magnification will not resolve two images that are closer than the resolution of a telescope. The limit, called the Rayleigh criterion, depends on the diameter of the telescope's primary mirror and the wavelength of the light observed. For the visible light, the minimum separation of two objects which can just be resolved is given the equation on the leftside. "a" is the angular separation of two stars in arcseconds and D is the diameter of the primary mirror in inches. However, you may not actually be able to see two images this close together because of atmospheric conditions (seeing), relative brightness of the object, etc. |
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Magnification =(telescope focal length)/(eyepiece focal length) |
The magnifying power of a telescope is the number of times larger (in angular diameter) an object apprears through a telescope than with the unaided eye. Magnifying power is determined by the focal length of both the telescope and the eyepiece used (measure in the same units). A shorter focal length eyepiece gives greater magnification. |
| Focal Length | For a simple mirro, the focal length is the distance between that mirror and the place where the image is formed (i.e., the focal plane). In a telescope with more than one optical element(or mirror), the effective focal length is often longer than the telescope tube itself. It is useful to know the focal length of the telescope or eyepiece that you are using. The focal length of the eyepieces are stamped on the viewing end of each eyepiece. |
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Scale =57.3°/focal length of telescope's primary mirror =206265"/focal length of telescope's primary mirror |
The scale at the focus of any astronomical telescop is the ratio of the angular size of an object in the sky to its image size with that telescope (i.e., how large the object would look if you were to photograph it with that telescope). The scale is constant for a particular telescope and depends only on the focal length of the primary mirror. The scale is usually expressed in units of degrees per millimeter (°/mm) or arcseconds per millimeter ("/mm). |
| Don't get confused magnification with angular resolution. The figure on the right shows that the angular resolutions which are determined by the diameter of a primary mirror can be different even though the magnifications which are determined by the combinations of primary mirrors and eyepices are same. |
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