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An instrument used in astronomical research to detect and measure the radio-frequency power coming from various directions in the sky. It consists of three complementary parts: the large reflecting surface that collects and focuses the incident radiation; the electronic receiver that amplifies and detects cosmic radio signals; and a data display device. From the ground, observations with radio telescopes must be made at wavelengths shorter than 100 ft (30 m), because of ionospheric attenuation, and longer than 0.04 in. (1 mm), because the very-short-wavelength radio radiation is absorbed by atmospheric H2O, CO2, and O3.
The fundamental principle of a radio telescope is identical to that of a reflecting telescope used at visual wavelengths. The incoming waves (radio or optical) are intercepted by a precise mirror and reflected to a common focal point. The shape of the reflecting surface or “dish” is important: the radio waves must arrive “in phase” at the focal point following their reflection from the dish; that is, the path length from the point of reflection to the focus must be exactly the same for all points on the dish. This restriction can be most simply satisfied if the shape of the reflecting surface is made paraboloidal; consequently, most modern radio telescopes have this shape (see illustration).

The 328-ft-diameter (100-m) radio telescope operated by the Max Planck Institut für Radioastronomie at Effelsberg, Germany. (Max Planck Insititut für Radioastronomie)
Once the radio waves are collected and brought together at the focal point of the telescope, they are in general still extremely weak. The incoming radio-frequency (rf) signals are first amplified at the focus 10 to 1000 times and then converted to a lower frequency, the intermediate frequency (i-f), that can be easily transmitted by cables from the focal point to the telescope-control building. There the i-f is further amplified, and the signal is detected and displayed in the manner the astronomer finds most suited to the particular investigation.
The types of astronomical objects that emit radio-frequency radiation and hence can be studied by radio astronomers are of such a diverse nature that a variety of radio telescopes and receiving equipment are necessary for a modern radio observatory. Two general astronomical considerations dictate what instruments are needed: first, radio telescopes should have the highest possible angular resolution so that the small-scale details of radio sources can be studied; second, the radio receivers should be extremely sensitive to the very weak signals emitted by cosmic radio sources.
The ultimate in angular resolution is achieved by the technique of very-long-baseline interferometry (VLBI), in which one simultaneously utilizes radio telescopes separated by thousands of miles. Data are acquired independently at each telescope and recorded on video tape. Precise time markings are made on the tape using hydrogen maser clocks. After the data are recorded, the video tapes from the separate telescopes are brought together; the time markings on the individual tapes are aligned, and data taken at precisely the same times can be compared and analyzed. Such VLBI techniques have achieved angular resolutions of about 0.0003 second of arc. See also Astronomy.
| WordNet: radio telescope |
The noun has one meaning:
Meaning #1:
astronomical telescope that picks up electromagnetic radiations in the radio-frequency range from extra-terrestrial sources
Synonym: radio reflector
| Wikipedia: Radio telescope |
A radio telescope is a form of directional radio antenna used in radio astronomy. The same types of antennas are also used in tracking and collecting data from satellites and space probes. In their astronomical role they differ from optical telescopes in that they operate in the radio frequency portion of the electromagnetic spectrum where they can detect and collect data on radio sources. Radio telescopes are typically large parabolic ("dish") antennas used singly or in an array. Radio observatories are preferentially located far from major centers of population in order to avoid electromagnetic interference (EMI) from radio, TV, radar, and other EMI emitting devices. This is similar to the locating of optical telescopes to avoid light pollution, with the difference being that radio observatories are often placed in valleys to further shield them from EMI as opposed to clear air mountain tops for optical observatories.
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The first radio antenna used to identify an astronomical radio source was one built by Karl Guthe Jansky, an engineer with Bell Telephone Laboratories, in 1931. Jansky was assigned the job of identifying sources of static that might interfere with radio telephone service. Jansky's antenna was an array of dipoles and reflectors designed to receive short wave radio signals at a frequency of 20.5 MHz (wavelength about 14.6 m). It was mounted on a turntable that allowed it to rotate in any direction, earning it the name "Jansky's merry-go-round". It had a diameter of approximately 100 ft (30 m). and stood 20 ft (6 m). tall. By rotating the antenna on a set of four Ford Model-T tires, the direction of the received interfering radio source (static) could be pinpointed. A small shed to the side of the antenna housed an analog pen-and-paper recording system. After recording signals from all directions for several months, Jansky eventually categorized them into three types of static: nearby thunderstorms, distant thunderstorms, and a faint steady hiss of unknown origin. Jansky finally determined that the "faint hiss" repeated on a cycle of 23 hours and 56 minutes. This period is the length of an astronomical sidereal day, the time it takes any "fixed" object located on the celestial sphere to come back to the same location in the sky. Thus Jansky suspected that the hiss originated well beyond the Earth's atmosphere, and by comparing his observations with optical astronomical maps, Jansky concluded that the radiation was coming from the Milky Way Galaxy and was strongest in the direction of the center of the galaxy, in the constellation of Sagittarius.
An amateur, Grote Reber, was one of the pioneers of what became known as radio astronomy when he built the first parabolic "dish" radio telescope (9 m in diameter) in his back yard in Illinois in 1937. He was instrumental in repeating Karl Guthe Jansky's pioneering but somewhat simple work at higher frequencies, and he went on to conduct the first sky survey at VHF radio frequencies. The rapid development of radar technology during World War II was easily translated into radio astronomy technology after the war, and the field of radio astronomy began to blossom.
The range of frequencies in the electromagnetic spectrum that makes up the radio spectrum is very large. This means that the types of antennas that are used as radio telescopes vary widely in design, size, and configuration. At wavelengths of 30 meters to 3 meters (10 MHz - 100 MHz), they are generally either directional antenna arrays similar to "TV antennas" or large stationary reflectors with moveable focal points. Since the wavelengths being observed with these types of antennas are so long, the "reflector" surfaces can be constructed from coarse wire mesh such as chicken wire.[1] At shorter wavelengths “dish” style radio telescopes predominate. The angular resolution of a dish style antenna is determined by the diameter of the dish expressed as a number of wavelengths of the electromagnetic radiation being observed. This dictates the size of the dish a radio telescope needs in order to have a useful resolution. Radio telescopes operating at wavelengths of 3 meters to 30 cm (100 MHz to 1 GHz) are usually well over 100 meters in diameter. Telescopes working at wavelengths above 30 cm (1 GHz) range in size from 3 to 90 meters in diameter.
The world's largest filled-aperture telescope (i.e., a full dish) is the Arecibo radio telescope located in Arecibo, Puerto Rico, whose 305-meter dish is fixed in the ground. The antenna beam is steerable (by means of a moving receiver) within about 20° of the zenith. The largest individual radio telescope of any kind is the RATAN-600 located near Nizhny Arkhyz, Russia, which consists of a 576-meter circle of rectangular radio reflectors, each of which can be pointed towards a central conical receiver.
The largest radio telescope in Europe is the 100-meter diameter antenna in Effelsberg, Germany, which also was the world's largest fully-steerable telescope for 30 years until the slightly larger Green Bank Telescope was opened in West Virginia, United States, in 2000. The third-largest fully-steerable radio telescope is the 76-metre Lovell Telescope at Jodrell Bank Observatory in Cheshire, England.
A typical size of the single antenna of a radio telescope is 25 meters. Dozens of radio telescopes with comparable sizes are operated in radio observatories all over the world.
China officially started construction of the world's largest single-aperture radio telescope in 2009, the FAST.[2] The FAST, with a dish area as large as 30 football fields, will stand in a region of typical Karst depressions in Guizhou, and will be finished by 2013.
One of the most notable developments came in 1946 with the introduction of the technique called astronomical interferometry. Astronomical radio interferometers usually consist either of arrays of parabolic dishes (e.g. the One-Mile Telescope), arrays of one-dimensional antennas (e.g. the Molonglo Observatory Synthesis Telescope) or two-dimensional arrays of omni-directional dipoles (e.g. Tony Hewish's Pulsar Array). All of the telescopes in the array are widely separated and are usually connected together using coaxial cable, waveguide, optical fiber, or other type of transmission line. Recent advances in the stability of electronic oscillators also now permit interferometry to be carried out by independent recording of the signals at the various antennas, and then later correlating the recordings at some central processing facility. This process is known as VLBI (Very Long Baseline Interferometry). Interferometry does increase the total signal collected, but its primary purpose is to vastly increase the resolution through a process called Aperture synthesis. This technique works by superposing (interfering) the signal waves from the different telescopes on the principle that waves that coincide with the same phase will add to each other while two waves that have opposite phases will cancel each other out. This creates a combined telescope that is equivalent in resolution (though not in sensitivity) to a single antenna whose diameter is equal to the spacing of the antennas furthest apart in the array. In order to produce a high quality image, a large number of different separations between different telescopes are required (the projected separation between any two telescopes as seen from the radio source is called a baseline) - as many different baselines as possible are required in order to get a good quality image (For example the Very Large Array (VLA) near Socorro, New Mexico has 27 telescopes giving 351 independent baselines at once to achieve resolution of 0.2 arc seconds at 3 cm wavelengths[3]). Martin Ryle's group in Cambridge obtained a Nobel Prize for interferometry and aperture synthesis[4]. The Lloyd's mirror interferometer was also developed independently in 1946 by Joseph Pawsey's group at the University of Sydney[5]. In the early 1950s the Cambridge Interferometer mapped the radio sky to produce the famous 2C and 3C surveys of radio sources. The largest existing physically-connected radio telescope array is the Giant Metrewave Radio Telescope, located in Pune, India. A larger array, LOFAR (the 'LOw Frequency ARray') is currently being constructed in western Europe, consisting of 25 000 small antennas over an area several hundreds of kilometres in diameter. VLBI systems using post-observation processing have been constructed with antennas thousands of miles apart. Radio interferometers have also been used to obtain detailed images of the anisotropies and the polarization of the Cosmic Microwave Background, like the CBI interferometer in 2004.
Many astronomical objects are not only observable in visible light but also emit radiation at radio wavelengths. Besides observing energetic objects such as pulsars and quasars, radio telescopes are able to "image" most astronomical objects such as galaxies, nebulae, and even radio emissions from planets.
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