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Macmillan Dictionary of Astronomy PDF

443 Pages·1979·52.739 MB·English
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THE MACMILLAN DICTIONARY OF ASTRONOMY Contributors Rosamund L. Briggs, BSc Peter H. Cadogan, BSc, PhD Heather Couper, BSc, FRAS Charles A. Cross, MA, FRAS John Daintith, BSc, PhD Tony Dean, BSc, PhD, FRAS Peter Duffett-Smith, BSc, PhD, FRAS Professor Andrew Fabian, BSc, PhD, FRAS Peter Gill, FRAS Nigel Henbest, BSc, MSc, FRAS David W. Hughes, BSc, PhD, FRAS Garry E. Hunt, DSc, PhD, FIMA, FRAS, FMet.S, MBCS Valerie Illingworth, BSc, MPhil Professor Philip L. Marsden, BSc, PhD, FIP, FRAS Alan Pickup, FRAS James Pinfold, BSc, PhD Professor Ken Pounds, BSc, PhD, FRS, CBE Gareth Rees, BSc, PhD, FRAS Allan J. Willis, BSc, PhD, FRAS IOO&CCOOTIILIL&~ WllCCTrll@~&ffi'IT @1F ASTRONOMY SECOND EDITION VALERIE ILLINGWORTH M MACMILLAN PRESS LONDON © Laurence Urdang Associates Ltd 1979 Material for new edition © Market House Books Ltd 1985 All rights reserved. No part of this publication may be reproduced or transmitted, in any form or by any means, without permission First published 1979; second edition 1985 by THE MACMILLAN PRESS LTD London and Basingstoke Associated companies throughout the world British Library Cataloguing in Publication Data Macmillan dictionary of astronomy. - 2nd ed 1. Astronomy - Dictionaries 520' .3'21 QB14 ISBN 978-0-333-39243-0 ISBN 978-1-349-17803-2 (eBook) DOI 10.1007/978-1-349-17803-2 Prepared for automatic typesetting by Market House Books Ltd Aylesbury Preface The tremendous advances in astronomy in the past five years, combined with the enthusiastic reception of the original edition, have encouraged the publishers to call for this second edition of the Dictionary ofA stronomy. New and improved ground-based observational techniques and instruments and several highly successful astronomical satellites and planetary probes have produced a flood of information together with new and modified ideas about celestial objects. These advances in astronomy are described in the new dictionary: entries in the first edition have been updated, often extensively, and over 250 entries have been added, bringing the total to more than 2300. The dictionary contains several long entries in which a word of primary importance is defined and discussed and in which closely associated words, printed in italics, are also defined. In these and in the shorter entries, an asterisk (*) before a word or group of words indicates additional entries that the reader could consult for further information. Synonyms and abbrevia tions of entries are placed in brackets immediately following the headword. Tables at the back of the dictionary contain general information while tables and illustrations in the text relate to specific entries. I would like to express my thanks and appreciation to all those involved in the preparation of the second edition, especially the contributors who produced the new and updated entries and those at astronomical centres in the UK, Europe, and the USA who have readily supplied information on request. Valerie Illingworth November 1984 absorption spectrum A AA T. Abbrev. for Anglo-Australian and also for those falling at oblique telescope. angles on the lens or mirror surface. The four principal aberrations are Abell catalogue. The standard cata *chromatic aberration (lenses only), logue of rich *clusters of galaxies visi *spherical aberration, *coma, and ble from the northern hemisphere. It *astigmatism. *Curvature of field and was published by George Abell in *distortion are other aberrations. 1958. Chromatic aberration occurs when more than one wavelength is present aberration. I. (aberration of starlight). in the incident light beam. For light The apparent displacement in the po of a single wavelength, only the latter sition of a star due to the finite speed five aberrations occur. These image of light and to the motion of the ob defects may be reduced - but not server, which results primarily from completely eliminated - in an optical the earth's orbital motion around the system by a suitable choice of optical sun. It was discovered in 1729 by the materials, surface shape, and relative English astronomer James Bradley. positions of optical elements and Light appears to approach the observ stops. See also achromatic lens; cor er from a point that is displaced recting plate. slightly in the direction of the earth's 3. A defect in the image produced motion. The angular displacement, a, by an electronic system using magnet is given by the ratio vic, where v is ic or electronic lenses. the earth's orbital velocity and c is the speed of light. Using the earth's absolute magnitude. See magnitude. mean orbital speed gives the constant of aberration, equal to 20.4955 arc absolute temperature scale. See ther seconds. Over the course of a year, modynamic temperature scale. the star appears to move in a small ellipse around its mean position; the absolute zero. The zero value of the ellipse becomes a circle for a star at *thermodynamic temperature scale, the pole of the *ecliptic and a i.e. 0 K (-273.l5°C). Absolute zero is straight line for one on the ecliptic. the lowest temperature theoretically The maximum displacement, i.e. the possible. At absolute zero molecular semimajor axis of the ellipse, is 20.5 motion almost ceases. arc seconds. The aberration due to the earth's absorption lines, bands. See absorption orbital motion is sometimes termed spectrum. annual aberration to distinguish it from the very much smaller diurnal absorption nebula. See dark nebula. aberration that results from the earth's rotation on its axis. Compare annual absorption spectrum. A *spectrum that parallax. is produced when *electromagnetic ra 2. A defect in the image formed by diation has been absorbed by matter. a lens or curved mirror, seen as a Typically, absorption spectra are pro blurring and possible false coloration duced when radiation from an incan in the image. Aberrations occur for descent source, i.e. radiation with a all light rays lying off the optical axis *continuous spectrum, passes through abundance 2 cooler matter. Radiation is absorbed in a gravitational field. It is equal to (i.e. its intensity is diminished) at se GM/ R2, where G is the gravitational lective wavelengths so that a pattern constant and M and R are the mass of very narrow dips or of wider and radius of the planet. The acceler troughs - i.e. absorption lines or ation is thus independent of the mass bands - are superimposed on the of the accelerated object, i.e. it is the continuous spectrum. same for all bodies (neglecting air re The wavelengths at which absorp sistance) falling at the same point on tion occurs correspond to the energies the surface of the planet, satellite, etc. required to cause transitions of the On earth the standard value of the absorbing atoms or molecules from acceleration of gravity is 9.806 65 me lower *energy levels to higher levels. tres per second per second. The value In the hydrogen atom, for example, varies from place to place on the absorption of a photon with the re earth's surface because of different quired energy results in a 'jump' of distances to the earth's centre and the electron from its normal orbit to greater acceleration towards the equa one of higher energy (see hydrogen tor. In addition, it is affected by local spectrum). deposits of light or heavy materials. The absorption lines (or bands) of a star are produced when elements accretion (aggregation). The increase (or compounds) in the outermost lay in mass of a body by the addition of ers of the star absorb radiation from smaller bodies that collide and stick a continuous distribution of wave to it. The relative velocity of any two lengths generated at a lower level in colliding bodies must be low enough the star. Basically the same elements for them to coalesce on impact rather occur in stars. Since each element has than fly apart. Once a large enough a characteristic pattern of absorption body forms, its gravitational attrac lines for any particular temperature tion accelerates the accretion process. (and pressure) range, there are several Accretion is now assumed to have different types of stellar spectra de had an important role in the forma pending on the surface temperature of tion of the planets from swarms of the star. See spectral types. See also dust grains. See solar system, origin. emission spectrum. accretion disc. See black hole; mass abundance. See cosmic abundance. transfer. Acamar. See Eridanus. Achemar (a Eri). A conspicuous blu ish-white star that is the brightest in acceleration. 1. Oinear acceleration). the constellation Eridanus. Illy: 0.5; Symbol: a. The rate of increase of ve M_.: -2.2; spectral type: B5 V; dis locity with time, measured in metres tance: 35 pc. per second per second (m s-2), etc. 2. (angular acceleration). Symbol: a. Achilles. The first member of the The rate of increase of *angular ve *Trojan group of *minor planets to locity with time, usually measured in be discovered, in 1906. It lies east of radians per second per second. Jupiter and precedes the latter in its orbit of the sun. See Table 3, acceleration of gravity. Symbol: g. The backmatter. acceleration to the centre of a planet (or other massive body such as a nat achondrite. Any of a class of *stony ural satellite) of an object falling free meteorites that lack the characteristic ly without air resistance, i.e. *chondrules of the *chondrites. They acceleration due to downward motion are usually more coarsely crystallized 3 active regions than the chondritic stones and are 1t 1s the radio-emitting lobes created more similar chemically and minera by *beams emanating from the pow logically to some terrestrial rocks. erhouse that are observed. There is They contain very little iron and nick mounting evidence that quasars and el. Seyferts are associated with spiral ga lactic structure while radio galaxies, achromatic lens (achromat). A two-ele BL Lac objects, and possibly N gal ment lens - a doublet - that greatly axies might represent activity in ellip reduces *chromatic aberration in an tical galaxies. optical system. The components, one Observations of the motions of converging and the other diverging in stars and gas in galaxies such as M87 action, are of different types of glass (see Virgo A) and NGC 4151 (see (i.e. they have different *refractive in Seyfert galaxy), in addition to theoret dices); the combination focuses two ical arguments (see quasar), strongly selected colours, say red and blue, at suggest that the energy output is de a common image plane with a small rived from the gravitational pot-ential spread in focal length for other of a supermassive *black hole: the en colours. The difference in optical ergy would arise from an accretion power (reciprocal of focal length) for disc of gases spiralling into the black the two colours in one element must hole. This gas could come from the cancel that in the other element. By a interstellar medium of a spiral galaxy suitable choice of glasses and surface (especially when perturbed by gravita curvatures, the doublet can be *apla tional effects in *interacting galaxies), natic as well as achromatic, so that from the tidal disruption of stars near three major aberrations are mini the black hole, or from flows of inter mized. galactic gas on to the central galaxy Residual colour effects in an achro of a *cluster of galaxies, as the gas mat can be further reduced by using cools (see Perseus cluster). a compound lens of three or more el ements - an apochromatic lens; each active optics. The techniques and element has an appropriate shape and technology by which any distortion, dispersive power so that three or arising from atmospheric effects, of a more colours can be focused in the *wavefront entering a telescope can same image plane. be sensed and information fed back to a deformable primary mirror whose acronical rising (or setting). The rising profile is continuously adjusted to (or setting) of a star at or just after compensate. This should in theory sunset. When the rising is acronical lead to diffraction-limited perform the setting is cosmic and vice versa. ance at all times (see Airy disc). Acrux. See Alpha Crucis. active prominence. See prominences. active galaxy. A galaxy that is emit active-region filament. See prom- ting unusually large amounts of ener inences. gy from a very compact central source. (A separate category, active regions. Regions of intense lo *starburst galaxy, is now employed calized magnetic field on the sun that for a galaxy where a high infrared lu extend from the *photosphere, minosity arises from intense star for through the *chromosphere, to the mati'on.) This central powerhouse may *corona. They may encompass a vari be observed directly, as in *Seyfert ety of phenomena, such as *sunspots, galaxies, *N galaxies, '~<BL Lac ob *faculae/*plages, *filaments (or jects, or *quasars; in *radio galaxies *prominences), and *flares, and are active sun 4 characterized by enhanced emission of seconds per century. This agrees al radiation at x-ray, ultraviolet, and ra most exactly with the discrepancy be dio wavelengths. tween the experimentally determined value for the advance and that pre active sun. The term applied to the dicted by classical Newtonian me sun around the maximum of the chanics. It was therefore an important *sunspot cycle, when the profusion of confirmation of general relativity. Re *active regions ensures a high level of cent measurements of the advance of *solar activity. Compare quiet sun. the perihelia of Venus and Earth have also been very close to Einstein's pre Adhara (e CMa). A very luminous re dicted values for those planets. mote blue-white giant that is the sec ond brightest star in the constellation aeon. A period of one thousand mil Canis Major. It is a visual double star lion years: 109 years. with an 8th-magnitude companion at a fixed separation of 8". IDy: 1.5; Mv: aerial. See antenna. -5.0; spectral type: B2 II; distance: 200 pc. aerolite. See stony meteorite. adiabatic process. A process that takes aeronomy. The physics and chemistry place in a system with no heat trans of the upper atmosphere of the earth, fer to or from the system. In general, i.e. its temperature, density, motions, a temperature change usually occurs composition, chemical processes, reac in an adiabatic process. tions to solar and cosmic radiation, etc. The term has been extended to adiabatic theory. See galaxies, forma include the physics and chemistry of tion and evolution. the atmospheres of the other planets. Adonis. A member of the *Apollo aerospace. The earth's atmosphere group of *minor planets. Discovered and the space beyond. in 1936 when it passed 0.015 AU from the earth, it was not observed again until it was recovered in 1977. Ae stars. Hot stars of *spectral type Its *perihelion distance of 0.44 AU is A that in addition to the normal ab the fourth smallest among the minor sorption spectrum have bright emis planets. See Table 3, backmatter. sion lines of hydrogen. These lines are thought to arise in an expanding at advance of the perihelion. The gradual mospheric shell of matter lost from movement of the *perihelion of a the star. Like some *Be stars they are planet's elliptical orbit in the same di probably similar to *T Tauri stars ex rection as that of the planet's orbital cept that they have larger masses. motion. This advance results from the slow rotation of the major axis of the afocal system. An optical system in planet's orbit due to gravitational dis which both the object and the second turbances by other planets and to the ary image are infinitely distant. It is curvature of *spacetime around the the usual adjustment in a simple re sun. The small contribution from the fracting telescope and is produced curvature of spacetime was predicted when the objective and eyepiece by Einstein's general theory of *rela lenses are separated by the sum of tivity. their focal lengths: the lenses are then The value of this relativistic contri confocal. bution towards the advance of the perihelion of Mercury is about 43 arc AG catalogue. See AGK.

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