38 r jsMOa.temperature <strong>the</strong>y now possess, and which we designate as76° of a mercury <strong>the</strong>rmometer, had a temperature of ahout— 1400° or even many thousand times lower IIt still remains for us to consider two hypo<strong>the</strong>ses in relationto <strong>the</strong> existence of a fluid filling <strong>the</strong> regions of space,cf which one— <strong>the</strong> less firmly-based hypo<strong>the</strong>sis— -refers to <strong>the</strong>limited traiisijarency of <strong>the</strong> celestial regions and <strong>the</strong> o<strong>the</strong>r,;founded on direct observation and pelding numerical results,is deduced from <strong>the</strong> regularly shortened periodsof revolutionof Encke's comet. Olbers in Bremen, and, as Struve has observed,Leys de Cheseaux at Geneva, eighty years earlier"^drew attention to <strong>the</strong> dilemma, that since we could not conceiveany point in <strong>the</strong> infinite regions of space unoccupied bya fixed star, i. e.,du sun, <strong>the</strong> entire vault of heaven must appearas luminous as our sun if light w^ere transmitted to usin perfect intensity; or, if such be not <strong>the</strong> case, we must assumethat light experiences a diminution of intensity in itspassage through space, this diminution being more excessivethan in <strong>the</strong> inverse ratio of <strong>the</strong> square of <strong>the</strong> distance. Aswe do not observe <strong>the</strong> whole heavens to be almost uniformlyillumined by such a radiance of light (a subject consideredby Halleyt in an hypo<strong>the</strong>sis which he subsequently rejected),<strong>the</strong> regions of space can not, according to Cheseaux, Olbers,and Struve, possess perfect and absolute transparency. T<strong>here</strong>sults obtained by iSir William Herschel from gauging <strong>the</strong>Bet) to <strong>the</strong> heating influence of <strong>the</strong> earth's radiation, and <strong>the</strong> coolingpower of its own into space, woukl — indicate a medium temperature betweenthat of <strong>the</strong> celestial spaces 132^( Fahr.) and that of <strong>the</strong> earth'ssurface below it, 82° Fahr., at <strong>the</strong> equator, 3p Fahr., in <strong>the</strong> Polar Sea.Under — th.e equator, <strong>the</strong>n, it would stand, on <strong>the</strong> average, at 25° Fahr.,and in <strong>the</strong> Polar Sea at — 68° Fahr. The presence of <strong>the</strong> atmosp<strong>here</strong>tends to prevent <strong>the</strong> <strong>the</strong>rmometer so exposed from attaining <strong>the</strong>se extremelow temperatures: first, by imparting heat by conduction ;secjndly,by impeding radiation outward." Sir John Herschel, in <strong>the</strong>—Edinburgh Review, vol. 87, 1848, p. 222. "Si la chaleur des espacesplanetaires n'existait point, notre atmosp<strong>here</strong> eprouverait un refroidissement,dont on ne peut fix'jr la lim'.te. Probablement la vie des planteaet des animaux serait impassible a la surface du globe, on relcguce dansline etroite zone de cette surface." (Saigey, Physique du Globe, p. 77 .^* Traits de la Cometc de 1743. avec nne Addition sur la force de lahumiere et sa Propagation dans Vi<strong>the</strong>r, ct sur la distance des ^toiles fixes;par Loys de Cheseaux (1744). On <strong>the</strong> transparency of <strong>the</strong> regions ofspace, see Olbers, in Bode's Jnhrbuchfur 182G, s. 110-121 and Struve,;Etudes d'Asir. Stellairc, 1847, p. 83-93, and note 9.5.Compare alscSir John Herschel, Outlines of Astronomy, § 798, and Cosmos, vol i., p.151, 152.t Halley, On <strong>the</strong> InfinVij of <strong>the</strong> Sp<strong>here</strong> of Fixed Stars, in ihe PhiwsTransact., vol. xxxi., for t lo year 1720, p. 22-2(3.
RESISTING MEDIUM. 39Btars,^ and iVom his ingenious experimeu.ts on <strong>the</strong> space-penetratingpower of his great telescopes, seem to show, that if<strong>the</strong> light of Sirius in its passage to us through a gaseous ore<strong>the</strong>real fluid loses only -g- ^Q-th of its intensity, this assumption,which gives <strong>the</strong> amount of <strong>the</strong> density of a fluid capableof diminishing light, would suffice to explain <strong>the</strong> phenomenaas <strong>the</strong>y manifest <strong>the</strong>mselves. Among <strong>the</strong> doubtsadvanced by <strong>the</strong> celebrated author of "The New Outlinesof Astronomy" against <strong>the</strong> views of Olbers and Struvc, oneof <strong>the</strong> most importantis that his twenty-feet telescope shows,tliroughout <strong>the</strong> greater portion of <strong>the</strong> Milky Way in both hemisp<strong>here</strong>s,<strong>the</strong> smallest stars projected on a black ground. fA better proof, and one based, as we have already stated,upon direct observation of <strong>the</strong> existence of a resisting fluid, ^is alTorded by Encke's comet, and by <strong>the</strong> ingenious and importantconclusion to which my friend Avas led in his observationson this body. This resisting medium miist, however,be regarded as ditferent from <strong>the</strong> all-penetrating light-e<strong>the</strong>r,because <strong>the</strong> former is only capable of ofiering resistance inasmuchas it can not penetrate through solid matter. Theseobservations require <strong>the</strong> assumption of a tangential force toexplain <strong>the</strong> diminished period of revolution (<strong>the</strong> diminishedmajor axis of <strong>the</strong> ellipse), and this is most directly afiordedby <strong>the</strong> hypo<strong>the</strong>sis of a resisting fluid. § The greatest action* Coamos, vol. i., p. SG, 87.T "Throughout by far ihe larger portion of <strong>the</strong> extent of <strong>the</strong> MilkyWay ill botli hemisp<strong>here</strong>s, <strong>the</strong> general blackness (jf <strong>the</strong> ground of <strong>the</strong>heavens, on which its stars are projected .... In tliose regions w<strong>here</strong><strong>the</strong> zone is clearly resolved into stars, well separated, and seen projectedon a hind: ground, and w<strong>here</strong> we look out beyond <strong>the</strong>m into space.. . ."— Sir John Herschel, Outlines of As/'r., p. .537, 539.+ Cosmos, vol. i,, p. 8"), 86, 107; compare also Laplace, Essai Philosophiquesur les ProbabilUes, 1825, p. 133; Arago, in <strong>the</strong> Anmiaire d?iBureau des Long, pour 1832, p. 188, pour 183G, \>. 216; and Sir JohnHerschel, Outlines of Astr., § 577.^ The oscillatory movement of <strong>the</strong> emanations from <strong>the</strong> bead of somecomets, as in tliat of 1744, and in Halley's, as observed by Bessel, between<strong>the</strong> 12th and 22d of October, 1835 (Schumacher, Astron. Nachr.,Nos. 300, 302, § 185, 232), "may indeed, in <strong>the</strong> case of some individualsof this class of cosmical bodies, exert an influence on <strong>the</strong> translatoryand rotatory motion, and lead us to infer <strong>the</strong> action of polar forces("$ 201, 229), which differ from <strong>the</strong>ordinary attracting force of <strong>the</strong> sun;''but <strong>the</strong> regular acceleration observable for sixty-three years in Encke'spomet (whose period of revolution is 3^ years), can not be regarded as<strong>the</strong> result of incidental emanations. Compare, on this cosmically importantsubject, Bessel, in Schum.. Astron. Nachr., No. 289, s. G, andNo. 310, s. 345-350, with Encke's Treatise on <strong>the</strong> hypo<strong>the</strong>sis of Iho rf>slstliiic mc'dium, in Schum., No. 305. s. 285-274
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STELLAR LIGHT. 81)to such views bec
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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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