40 COSMOS.is manifested during <strong>the</strong> twenty-five days immedia'.ely pro»ceding and succeeding <strong>the</strong> comet's perihelion passage. Thevalue of <strong>the</strong> constant is <strong>the</strong>refore somewhat different, becausein <strong>the</strong> neighborhood of <strong>the</strong> sun <strong>the</strong> highly attenuated butstill gravitating strata of <strong>the</strong> resisting fluid -are denser. Gibersmaintained"^ that this fluid could not be at rest, butmust rotate directly round <strong>the</strong> sun, and <strong>the</strong>refore <strong>the</strong> resistanceoffered to retrograde comets, like Halley's, must differwholly from that opposed to those comets having a directcourse, like Encke's. The perturbations of comets havinglong periods of revolution; and <strong>the</strong> difference of <strong>the</strong>ir magnitudes and sizes, complicate <strong>the</strong> results, and render it dilf?-cult to determine what is ascribable to individual forces.The gaseous matter constituting <strong>the</strong> belt of <strong>the</strong> zodiacallight may, as Sir John Herschelf expresses it, be merely <strong>the</strong>denser portion of this comet-resisting medium. Although itmay be shown that all nebulae are crowded stellar masses,indistinctly visible, it is certain that innumerable comets fill<strong>the</strong> regions of space with matter through <strong>the</strong> evaporation of<strong>the</strong>ir tails, some of which have a length of 56,000,000 ofmiles. Arago has ingeniously shown, on optical grounds, $that <strong>the</strong> variable stars which always exhibit white lightwithout any change of color in <strong>the</strong>ir periodical phases, mightafford a means of determining <strong>the</strong> superior hmit of <strong>the</strong> densityto be assunaed for cosmic al e<strong>the</strong>r, if we supposeit to beequal to gaseous terrestrial fluids in itspower of refraction.The question of <strong>the</strong> existence of an e<strong>the</strong>real fluid filling<strong>the</strong> regions of space is closely connected with one warmlyagitated by "Wollaston,^ in reference to <strong>the</strong> definite limit of<strong>the</strong> atmosp<strong>here</strong>— a limit which must necessarily exist at <strong>the</strong>elevation w<strong>here</strong> <strong>the</strong> specific elasticity of <strong>the</strong> air is equipoisedby <strong>the</strong> force of gravity. Faraday's ingenious experiments on* Olbers, in Schum., Asir. NacJir., No. 268, s. 58.t Outlines of Astronomy , ^ 55G, 597.X ^^ En assimilant la watiere tres rare qui rempllt les espaces cilesteiquant a ses proprietes refringcntes aux gas terrestres, la density de cettimatiere nz saurait depasscr nne certaine limite dont les observations deeiloilcs chcngeantes, p. e. cellcs d'' Algol ou de (3 de Persic, peuvent assignerla valeur?^— Arago, in <strong>the</strong> Annnaire pour 1842, p. 336-345." On comparing <strong>the</strong> extremely rare matter occupying <strong>the</strong> regions oif space withterrestrial gases, in respect to its refractive properties, we shall find that<strong>the</strong> density of this matter can not exceed a definite limit, whose valuemay be obtained from observations of variable stars, as, for instance,Algol or (3 Tersei."i <strong>See</strong> WoWaRton, Philos. Transact, for 1822. p 80' Sir.Tnlin TIerschelcyp. cU., ^M, 36.
FIRST TELESCOPE. 41<strong>the</strong> limits of an atmosp<strong>here</strong> of mercury (that is, <strong>the</strong> elevationat which mercmial vapors precipitated on gold leaf ceaseperceptibly to rise in an air-tilled space) have given considerableweight to <strong>the</strong> assumption of a definite surface of <strong>the</strong>atmosp<strong>here</strong> " similar to <strong>the</strong> surface of <strong>the</strong> sea." Can anygaseous particles belonging to <strong>the</strong> region of space blend withour atmosp<strong>here</strong> and produce meteorological changes Newton*"inclined to <strong>the</strong> idea that such might be <strong>the</strong> case. If?we regard falling stars and meteoric stones as planetary as-that in <strong>the</strong> streamsteroids, we may be allowed to conjectureof <strong>the</strong> so-called JNTovember phenomena,! when, as in 1799,1833, and 1S34, myriads of falling stars traversed <strong>the</strong> vaultof heaven, and nor<strong>the</strong>rn liglitswere simultaneously observed,our atmosp<strong>here</strong> may have received from <strong>the</strong> regions of spacesome elements foreign to it, which were capable of excitingelectro-magnetic processes.II.NATURAL AND TELESCOPIC VISION.—SCINTILLATION OF THE STARS—VELOCITY OF LIGHT.—RESULTS OF PHOTOMETRY.The increased power of vision yielded nearly two hundredand fifty years ago by <strong>the</strong> invention of <strong>the</strong> telescope, has affordedto <strong>the</strong> eye, as <strong>the</strong> organ of sensuous cosmical contemplation, <strong>the</strong> noblest of all aids toward a knowledge of <strong>the</strong>contents of space, and tlie investigation of <strong>the</strong> configuration,ph^^sical character, and masses of <strong>the</strong> planets and <strong>the</strong>ir satellites.The first telescope was constructed in 1608, sevenyears after <strong>the</strong> death of <strong>the</strong> great observer, Tycho Brahe.Its earliest fruits were <strong>the</strong> successive discovery of <strong>the</strong> satellitesof Jupiter, <strong>the</strong> Sun's spots, <strong>the</strong> crescent shape of Venus,<strong>the</strong> ring of Saturn as a triple planetary formation (planetatergeminus), telescopic stellar swarms, and <strong>the</strong> nel3ulae inAndromeda. $ In 163-1, <strong>the</strong> French astronomer Morin, eminentfor his observations on longitude, first conceived <strong>the</strong> ideaof mounting a telescope on <strong>the</strong> index bar of an instrumentof measurement, and seeking to discover Arcturus by day.^* Newton, Princ. Ma<strong>the</strong>m., t. iii. (1760), p. G71: "Tapores qui ejBole et stellis fixis et caiidis cometarum oriuutur, iiicidere possvnt in at>"mosphaeras planetarumt Cosmos, vol. i., p. 124-135X <strong>See</strong> Cosmos, vol. ii., p. 317-335, with notes.§ Dclanibre, Histoire de C Astronomie Moderne, torn, ii., p. 255, 239
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- Page 13 and 14: INTRODUCTION. 7tiiieiital masses in
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MAGNITUDES OF STARSDir;40 stars of
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ilOTOMETRIC METHODS. 1)3ing (in fro
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HOTOMETR'i'. 95Sir Jolin Herscliel
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PHOTOMETRY. 97his own words, the re
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PHOTOMETRIC SCALE. 99raoTOMi:TRic a
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PHOTOMETRIC SCALE. 101Stars of the
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tt.i.rfUMBER, DISTRIBUTION, AND COL
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NUMBER OF THE FIXED STARS. iOlHersc
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NUMliER OF TUB FIXED STARS. 101Tst
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NUMBER OF THE FIXED STARS. 109Star
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EARLY CATA'.OGUES. Illthat of Tycho
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PROGRESS OF ASTRONOMY. 113the labor
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STAR CATALOGUES 115La Caille, Tobia
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DISTRIBUTION OF THE FIXED STARS. 11
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ZODIACAL SIGNS. 119groups the for.n
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i,ODlACAL SIGNS. 121passage, pDjbaW
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AcliillesTHE FIXED STARS 123to tlio
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THE FIXED STARS. 123idea of transpa
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VELOCITY OF LIGHT.IS'/tne eye,diflr
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RAYS OF THE STARS. 12Switli a needl
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COLOU OF THE STARS. 131ifiope, ill
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SIRIU3. 133gjini,who invariably fol
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THE COLOR OF THE STARS 135Btars, St
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SOUTHERN STARS.ISTEentatioiis of De
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DISTRIBUTION OF STARS.13Sbeen made
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CLUSTERS OF STARS. 141tail of Scorj
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CLUSTERS OF STAR3. 143of Cambridge,
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MILKY WAY. 145be asciibed to irreso
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MILKY WA /. 147tioii of the souther
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MILKY WAY. 149of Ceplieus, and ther
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NEW STARS. 151ft1rat\im. is about e
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A^VV STARS. 153diminisii,. and the
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etweenTEMPORARY STARS. 155transitio
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TEMPORARY STARS.It>'/{g) March, 393
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TEMPORARY STARS. 159excitt
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N£VV STARS 161aetic process in the
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VANISHED STARS.1G3bricius as sudden
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PERIODICAL STARS. 165with uniform i
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VARIABLE STARS. 167That the periods
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VARIABLE STARS. 169perioJs of the m
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VARIABLE STARS. 171have loDg' appea
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VARIABLE STARS.17Jright ascension a
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VARIABLE STARS. 175The Huctaations,
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VARIABLE STARS. 11^lU brightuess at
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VARIABLE STARS. 179to the observati
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VARIABLE STARS. 181served by liLn.
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PROPER MOTION OF THE STARS. 183cuns
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_PROPER iMOTION OF THE STARS. If 5t
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PROPER MOTION OF THE STARS. 187A la
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DISTANCES OF THE STARS.Ibllniibsima
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DISTANCES OF THE STARS.19Jfiords, "
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Fixed Star.DISTANCES OF THE STARS.
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PROPER MOTION OF THE STARS. . 195li
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MOTION OF THE STARS. 197question na
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DOUBLE STARS. 199not the place to d
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OOUBLL STARS. 201distnnce from each
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DOUBLE &TAR3. 203The importance of
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DOUBLE STARS20ldation of this impor
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DOUBLE STARS 20*7most recent gives
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DOUBLE STARS.!2USstances In which a
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DOUBLE STARS.21 JOrion, we have a c
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DOUBLE STARS.213Elements ofthe Orbi
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neINDEX.Cosiiiical vnpor, question
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218 INDEX./^i-nerical rcctilta exce
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