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the¡¡suggestions¡¡presently¡¡to¡¡be¡¡set¡¡forth¡¡concerning¡¡the¡¡Unseen¡¡World£»¡¡and¡¡we¡¡shall¡¡find¡¡it¡¡most¡¡convenient¡¡to¡¡begin£»¡¡like¡¡our¡¡authors£»¡¡with¡¡a¡¡brief¡¡statement¡¡of¡¡what¡¡the¡¡principle¡¡of¡¡continuity¡¡teaches¡¡as¡¡to¡¡the¡¡proximate¡¡beginning¡¡and¡¡end¡¡of¡¡the¡¡visible¡¡universe¡£¡¡I¡¡shall¡¡in¡¡the¡¡main¡¡set¡¡down¡¡only¡¡results£»¡¡having¡¡elsewhere£§2£§¡¡given¡¡a¡¡simple¡¡exposition¡¡of¡¡the¡¡arguments¡¡upon¡¡which¡¡these¡¡results¡¡are¡¡founded¡£

£§1£§¡¡The¡¡Unseen¡¡Universe£»¡¡or£»¡¡Physical¡¡Speculations¡¡on¡¡a¡¡Future¡¡State¡£¡¡£§Attributed¡¡to¡¡Professors¡¡TAIT¡¡and¡¡BALFOUR¡¡STEWART¡££§¡¡New¡¡York£º¡¡Macmillan¡¡&¡¡Co¡£¡¡1875¡£¡¡8vo¡£¡¡pp¡£¡¡212¡£

£§2£§¡¡Outlines¡¡of¡¡Cosmic¡¡Philosophy£»¡¡based¡¡on¡¡the¡¡Doctrine¡¡of¡¡Evolution¡£¡¡Boston£º¡¡J¡£¡¡R¡£¡¡Osgood¡¡&¡¡Co¡£¡¡1875¡£¡¡2¡¡vols¡£¡¡8vo¡£


The¡¡first¡¡great¡¡cosmological¡¡speculation¡¡which¡¡has¡¡been¡¡raised¡¡quite¡¡above¡¡the¡¡plane¡¡of¡¡guesswork¡¡by¡¡making¡¡no¡¡other¡¡assumption¡¡than¡¡that¡¡of¡¡the¡¡uniformity¡¡of¡¡nature£»¡¡is¡¡the¡¡well¡­known¡¡Nebular¡¡Hypothesis¡£¡¡Every¡¡astronomer¡¡knows¡¡that¡¡the¡¡earth£»¡¡like¡¡all¡¡other¡¡cosmical¡¡bodies¡¡which¡¡are¡¡flattened¡¡at¡¡the¡¡poles£»¡¡was¡¡formerly¡¡a¡¡mass¡¡of¡¡fluid£»¡¡and¡¡consequently¡¡filled¡¡a¡¡much¡¡larger¡¡space¡¡than¡¡at¡¡present¡£¡¡It¡¡is¡¡further¡¡agreed£»¡¡on¡¡all¡¡hands£»¡¡that¡¡the¡¡sun¡¡is¡¡a¡¡contracting¡¡body£»¡¡since¡¡there¡¡is¡¡no¡¡other¡¡possible¡¡way¡¡of¡¡accounting¡¡for¡¡the¡¡enormous¡¡quantity¡¡of¡¡heat¡¡which¡¡he¡¡generates¡£¡¡The¡¡so¡­called¡¡primeval¡¡nebula¡¡follows¡¡as¡¡a¡¡necessary¡¡inference¡¡from¡¡these¡¡facts¡£¡¡There¡¡was¡¡once¡¡a¡¡time¡¡when¡¡the¡¡earth¡¡was¡¡distended¡¡on¡¡all¡¡sides¡¡away¡¡out¡¡to¡¡the¡¡moon¡¡and¡¡beyond¡¡it£»¡¡so¡¡that¡¡the¡¡matter¡¡now¡¡contained¡¡in¡¡the¡¡moon¡¡was¡¡then¡¡a¡¡part¡¡of¡¡our¡¡equatorial¡¡zone¡£¡¡And¡¡at¡¡a¡¡still¡¡remoter¡¡date¡¡in¡¡the¡¡past£»¡¡the¡¡mass¡¡of¡¡the¡¡sun¡¡was¡¡diffused¡¡in¡¡every¡¡direction¡¡beyond¡¡the¡¡orbit¡¡of¡¡Neptune£»¡¡and¡¡no¡¡planet¡¡had¡¡an¡¡individual¡¡existence£»¡¡for¡¡all¡¡were¡¡indistinguishable¡¡parts¡¡of¡¡the¡¡solar¡¡mass¡£¡¡When¡¡the¡¡great¡¡mass¡¡of¡¡the¡¡sun£»¡¡increased¡¡by¡¡the¡¡relatively¡¡small¡¡mass¡¡of¡¡all¡¡the¡¡planets¡¡put¡¡together£»¡¡was¡¡spread¡¡out¡¡in¡¡this¡¡way£»¡¡it¡¡was¡¡a¡¡rare¡¡vapour¡¡or¡¡gas¡£¡¡At¡¡the¡¡period¡¡where¡¡the¡¡question¡¡is¡¡taken¡¡up¡¡in¡¡Laplace's¡¡treatment¡¡of¡¡the¡¡nebular¡¡theory£»¡¡the¡¡shape¡¡of¡¡this¡¡mass¡¡is¡¡regarded¡¡as¡¡spheroidal£»¡¡but¡¡at¡¡an¡¡earlier¡¡period¡¡its¡¡shape¡¡may¡¡well¡¡have¡¡been¡¡as¡¡irregular¡¡as¡¡that¡¡of¡¡any¡¡of¡¡the¡¡nebulae¡¡which¡¡we¡¡now¡¡see¡¡in¡¡distant¡¡parts¡¡of¡¡the¡¡heavens£»¡¡for£»¡¡whatever¡¡its¡¡primitive¡¡shape£»¡¡the¡¡equalization¡¡of¡¡its¡¡rotation¡¡would¡¡in¡¡time¡¡make¡¡it¡¡spheroidal¡£¡¡That¡¡the¡¡QUANTITY¡¡of¡¡rotation¡¡was¡¡the¡¡same¡¡then¡¡as¡¡now¡¡is¡¡unquestionable£»¡¡for¡¡no¡¡system¡¡of¡¡particles£»¡¡great¡¡or¡¡small£»¡¡can¡¡acquire¡¡or¡¡lose¡¡rotation¡¡by¡¡any¡¡action¡¡going¡¡on¡¡within¡¡itself£»¡¡any¡¡more¡¡than¡¡a¡¡man¡¡could¡¡pick¡¡himself¡¡up¡¡by¡¡his¡¡waistband¡¡and¡¡lift¡¡himself¡¡over¡¡a¡¡stone¡¡wale¡¡So¡¡that¡¡the¡¡primitive¡¡rotating¡¡spheroidal¡¡solar¡¡nebula¡¡is¡¡not¡¡a¡¡matter¡¡of¡¡assumption£»¡¡but¡¡is¡¡just¡¡what¡¡must¡¡once¡¡have¡¡existed£»¡¡provided¡¡there¡¡has¡¡been¡¡no¡¡breach¡¡of¡¡continuity¡¡in¡¡nature's¡¡operations¡£¡¡Now¡¡proceeding¡¡to¡¡reason¡¡back¡¡from¡¡the¡¡past¡¡to¡¡the¡¡present£»¡¡it¡¡has¡¡been¡¡shown¡¡that¡¡the¡¡abandonment¡¡of¡¡successive¡¡equatorial¡¡belts¡¡by¡¡the¡¡contracting¡¡solar¡¡mass¡¡must¡¡have¡¡ensued¡¡in¡¡accordance¡¡with¡¡known¡¡mechanical¡¡laws£»¡¡and¡¡in¡¡similar¡¡wise£»¡¡under¡¡ordinary¡¡circumstances¡£¡¡each¡¡belt¡¡must¡¡have¡¡parted¡¡into¡¡fragments£»¡¡and¡¡the¡¡fragments¡¡chasing¡¡each¡¡other¡¡around¡¡the¡¡same¡¡orbit£»¡¡must¡¡have¡¡at¡¡last¡¡coalesced¡¡into¡¡a¡¡spheroidal¡¡planet¡£¡¡Not¡¡only¡¡this£»¡¡but¡¡it¡¡has¡¡also¡¡been¡¡shown¡¡that¡¡as¡¡the¡¡result¡¡of¡¡such¡¡a¡¡process¡¡the¡¡relative¡¡sizes¡¡of¡¡the¡¡planets¡¡would¡¡be¡¡likely¡¡to¡¡take¡¡the¡¡order¡¡which¡¡they¡¡now¡¡follow£»¡¡that¡¡the¡¡ring¡¡immediately¡¡succeeding¡¡that¡¡of¡¡Jupiter¡¡would¡¡be¡¡likely¡¡to¡¡abort¡¡and¡¡produce¡¡a¡¡great¡¡number¡¡of¡¡tiny¡¡planets¡¡instead¡¡of¡¡one¡¡good¡­sized¡¡one£»¡¡that¡¡the¡¡outer¡¡planets¡¡would¡¡be¡¡likely¡¡to¡¡have¡¡many¡¡moons£»¡¡and¡¡that¡¡Saturn£»¡¡besides¡¡having¡¡the¡¡greatest¡¡number¡¡of¡¡moons£»¡¡would¡¡be¡¡likely¡¡to¡¡retain¡¡some¡¡of¡¡his¡¡inner¡¡rings¡¡unbroken£»¡¡that¡¡the¡¡earth¡¡would¡¡be¡¡likely¡¡to¡¡have¡¡a¡¡long¡¡day¡¡and¡¡Jupiter¡¡a¡¡short¡¡one£»¡¡that¡¡the¡¡extreme¡¡outer¡¡planets¡¡would¡¡be¡¡not¡¡unlikely¡¡to¡¡rotate¡¡in¡¡a¡¡retrograde¡¡direction£»¡¡and¡¡so¡¡on£»¡¡through¡¡a¡¡long¡¡list¡¡of¡¡interesting¡¡and¡¡striking¡¡details¡£¡¡Not¡¡only£»¡¡therefore£»¡¡are¡¡we¡¡driven¡¡to¡¡the¡¡inference¡¡that¡¡our¡¡solar¡¡system¡¡was¡¡once¡¡a¡¡vaporous¡¡nebula£»¡¡but¡¡we¡¡find¡¡that¡¡the¡¡mere¡¡contraction¡¡of¡¡such¡¡a¡¡nebula£»¡¡under¡¡the¡¡influence¡¡of¡¡the¡¡enormous¡¡mutual¡¡gravitation¡¡of¡¡its¡¡particles£»¡¡carries¡¡with¡¡it¡¡the¡¡explanation¡¡of¡¡both¡¡the¡¡more¡¡general¡¡and¡¡the¡¡more¡¡particular¡¡features¡¡of¡¡the¡¡present¡¡system¡£¡¡So¡¡that¡¡we¡¡may¡¡fairly¡¡regard¡¡this¡¡stupendous¡¡process¡¡as¡¡veritable¡¡matter¡¡of¡¡history£»¡¡while¡¡we¡¡proceed¡¡to¡¡study¡¡it¡¡under¡¡some¡¡further¡¡aspects¡¡and¡¡to¡¡consider¡¡what¡¡consequences¡¡are¡¡likely¡¡to¡¡follow¡£

Our¡¡attention¡¡should¡¡first¡¡be¡¡directed¡¡to¡¡the¡¡enormous¡¡waste¡¡of¡¡energy¡¡which¡¡has¡¡accompanied¡¡this¡¡contraction¡¡of¡¡the¡¡solar¡¡nebula¡£¡¡The¡¡first¡¡result¡¡of¡¡such¡¡a¡¡contraction¡¡is¡¡the¡¡generation¡¡of¡¡a¡¡great¡¡quantity¡¡of¡¡heat£»¡¡and¡¡when¡¡the¡¡heat¡¡thus¡¡generated¡¡has¡¡been¡¡lost¡¡by¡¡radiation¡¡into¡¡surrounding¡¡space¡¡it¡¡becomes¡¡possible¡¡for¡¡the¡¡contraction¡¡to¡¡continue¡£¡¡Thus£»¡¡as¡¡concentration¡¡goes¡¡on£»¡¡heat¡¡is¡¡incessantly¡¡generated¡¡and¡¡incessantly¡¡dissipated¡£¡¡How¡¡long¡¡this¡¡process¡¡is¡¡to¡¡endure¡¡depends¡¡chiefly¡¡on¡¡the¡¡size¡¡of¡¡the¡¡contracting¡¡mass£»¡¡as¡¡small¡¡bodies¡¡radiate¡¡heat¡¡much¡¡faster¡¡than

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But¡¡this¡¡is¡¡by¡¡no¡¡means¡¡the¡¡end¡¡of¡¡the¡¡story¡£¡¡When¡¡two¡¡bodies¡¡rush¡¡together£»¡¡each¡¡parts¡¡with¡¡some¡¡of¡¡its¡¡energy¡¡of¡¡motion£»¡¡and¡¡this¡¡lost¡¡energy¡¡of¡¡motion¡¡reappears¡¡as¡¡heat¡£¡¡In¡¡the¡¡concussion¡¡of¡¡two¡¡cosmical¡¡bodies£»¡¡like¡¡the¡¡sun¡¡and¡¡the¡¡earth£»¡¡an¡¡enormous¡¡quantity¡¡of¡¡motion¡¡is¡¡thus¡¡converted¡¡into¡¡heat¡£¡¡Now¡¡heat£»¡¡when¡¡not¡¡allowed¡¡to¡¡radiate£»¡¡or¡¡when¡¡generated¡¡faster¡¡than¡¡it¡¡can¡¡be¡¡radiated£»¡¡is¡¡transformed¡¡into¡¡motion¡¡of¡¡expansion¡£¡¡Hence¡¡the¡¡shock¡¡of¡¡sun¡¡and¡¡planet¡¡would¡¡at¡¡once¡¡result¡¡in¡¡the¡¡vaporization¡¡of¡¡both¡¡bodies£»¡¡and¡¡there¡¡can¡¡be¡¡no¡¡doubt¡¡that¡¡by¡¡the¡¡time¡¡the¡¡sun¡¡has¡¡absorbed¡¡the¡¡outermost¡¡of¡¡his¡¡attendant¡¡planets£»¡¡he¡¡will¡¡have¡¡resumed¡¡something¡¡like¡¡his¡¡original¡¡nebulous¡¡condition¡£¡¡He¡¡will¡¡have¡¡been¡¡dilated¡¡into¡¡a¡¡huge¡¡mass¡¡of¡¡vapour£»¡¡and¡¡will¡¡have¡¡become¡¡fit¡¡for¡¡a¡¡new¡¡process¡¡of¡¡contraction¡¡and¡¡for¡¡a¡¡new¡¡production¡¡of¡¡life¡­bearing¡¡planets¡£

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