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does¡¡not¡¡form¡¡independently¡¡but¡¡is¡¡formed¡¡by¡¡one¡¡of¡¡the¡¡fixed¡¡stars¡¡or



the¡¡planets¡£¡¡Then¡¡these¡¡stars¡¡appear¡¡to¡¡be¡¡fringed£»¡¡because¡¡matter



of¡¡this¡¡kind¡¡follows¡¡their¡¡course¡£¡¡In¡¡the¡¡same¡¡way£»¡¡a¡¡certain¡¡kind



of¡¡matter¡¡follows¡¡the¡¡sun£»¡¡and¡¡we¡¡explain¡¡the¡¡halo¡¡as¡¡a¡¡reflection



from¡¡it¡¡when¡¡the¡¡air¡¡is¡¡of¡¡the¡¡right¡¡constitution¡£¡¡Now¡¡we¡¡must



assume¡¡that¡¡what¡¡happens¡¡in¡¡the¡¡case¡¡of¡¡the¡¡stars¡¡severally¡¡happens¡¡in



the¡¡case¡¡of¡¡the¡¡whole¡¡of¡¡the¡¡heavens¡¡and¡¡all¡¡the¡¡upper¡¡motion¡£¡¡For



it¡¡is¡¡natural¡¡to¡¡suppose¡¡that£»¡¡if¡¡the¡¡motion¡¡of¡¡a¡¡single¡¡star



excites¡¡a¡¡flame£»¡¡that¡¡of¡¡all¡¡the¡¡stars¡¡should¡¡have¡¡a¡¡similar¡¡result£»



and¡¡especially¡¡in¡¡that¡¡region¡¡in¡¡which¡¡the¡¡stars¡¡are¡¡biggest¡¡and



most¡¡numerous¡¡and¡¡nearest¡¡to¡¡one¡¡another¡£¡¡Now¡¡the¡¡circle¡¡of¡¡the¡¡zodiac



dissolves¡¡this¡¡kind¡¡of¡¡matter¡¡because¡¡of¡¡the¡¡motion¡¡of¡¡the¡¡sun¡¡and¡¡the



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tropic¡¡circles¡£¡¡Again£»¡¡no¡¡fringe¡¡appears¡¡round¡¡the¡¡sun¡¡or¡¡moon£º¡¡for



they¡¡dissolve¡¡such¡¡matter¡¡too¡¡quickly¡¡to¡¡admit¡¡of¡¡its¡¡formation¡£¡¡But



this¡¡circle¡¡in¡¡which¡¡the¡¡milky¡¡way¡¡appears¡¡to¡¡our¡¡sight¡¡is¡¡the



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biggest¡¡and¡¡brightest¡¡constellations¡¡and¡¡also¡¡of¡¡what¡¡called



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for¡¡these¡¡reasons¡¡all¡¡this¡¡matter¡¡is¡¡continually¡¡and¡¡ceaselessly



collecting¡¡there¡£¡¡A¡¡proof¡¡of¡¡the¡¡theory¡¡is¡¡this£º¡¡In¡¡the¡¡circle



itself¡¡the¡¡light¡¡is¡¡stronger¡¡in¡¡that¡¡half¡¡where¡¡the¡¡milky¡¡way¡¡is



divided£»¡¡and¡¡in¡¡it¡¡the¡¡constellations¡¡are¡¡more¡¡numerous¡¡and¡¡closer



to¡¡one¡¡another¡¡than¡¡in¡¡the¡¡other¡¡half£»¡¡which¡¡shows¡¡that¡¡the¡¡cause¡¡of



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it¡¡is¡¡found¡¡in¡¡the¡¡circle¡¡in¡¡which¡¡there¡¡are¡¡most¡¡constellations¡¡and



at¡¡that¡¡point¡¡in¡¡the¡¡circle¡¡at¡¡which¡¡they¡¡are¡¡densest¡¡and¡¡contain



the¡¡biggest¡¡and¡¡the¡¡most¡¡stars£»¡¡it¡¡is¡¡natural¡¡to¡¡suppose¡¡that¡¡they¡¡are



the¡¡true¡¡cause¡¡of¡¡the¡¡affection¡¡in¡¡question¡£¡¡The¡¡circle¡¡and¡¡the



constellations¡¡in¡¡it¡¡may¡¡be¡¡seen¡¡in¡¡the¡¡diagram¡£¡¡The¡¡so¡­called



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but¡¡if¡¡you¡¡look¡¡up¡¡to¡¡the¡¡sky¡¡the¡¡point¡¡is¡¡clear¡£¡¡For¡¡in¡¡this¡¡circle



alone¡¡are¡¡the¡¡intervals¡¡full¡¡of¡¡these¡¡stars£º¡¡in¡¡the¡¡other¡¡circles



there¡¡are¡¡obvious¡¡gaps¡£¡¡Hence¡¡if¡¡we¡¡accept¡¡the¡¡cause¡¡assigned¡¡for



the¡¡appearance¡¡of¡¡comets¡¡as¡¡plausible¡¡we¡¡must¡¡assume¡¡that¡¡the¡¡same



kind¡¡of¡¡thing¡¡holds¡¡good¡¡of¡¡the¡¡milky¡¡way¡£¡¡For¡¡the¡¡fringe¡¡which¡¡in¡¡the



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being¡¡separated¡¡off¡¡and¡¡gathered¡¡into¡¡this¡¡region¡£



¡¡¡¡We¡¡have¡¡now¡¡explained¡¡the¡¡phenomena¡¡that¡¡occur¡¡in¡¡that¡¡part¡¡of¡¡the



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¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡9







¡¡¡¡Let¡¡us¡¡go¡¡on¡¡to¡¡treat¡¡of¡¡the¡¡region¡¡which¡¡follows¡¡next¡¡in¡¡order



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common¡¡to¡¡water¡¡and¡¡air£»¡¡and¡¡the¡¡processes¡¡attending¡¡the¡¡formation



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it¡¡approaches¡¡or¡¡recedes£»¡¡obviously¡¡causes¡¡dissipation¡¡and



condensation¡¡and¡¡so¡¡gives¡¡rise¡¡to¡¡generation¡¡and¡¡destruction¡£¡¡Now



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And¡¡after¡¡the¡¡water¡¡has¡¡formed¡¡it¡¡falls¡¡down¡¡again¡¡to¡¡the¡¡earth¡£



¡¡¡¡The¡¡exhalation¡¡of¡¡water¡¡is¡¡vapour£º¡¡air¡¡condensing¡¡into¡¡water¡¡is



cloud¡£¡¡Mist¡¡is¡¡what¡¡is¡¡left¡¡over¡¡when¡¡a¡¡cloud¡¡condenses¡¡into¡¡water£»



and¡¡is¡¡therefore¡¡rather¡¡a¡¡sign¡¡of¡¡fine¡¡weather¡¡than¡¡of¡¡rain£»¡¡for



mist¡¡might¡¡be¡¡called¡¡a¡¡barren¡¡cloud¡£¡¡So¡¡we¡¡get¡¡a¡¡circular¡¡process¡¡that



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this¡¡side¡¡or¡¡that£»¡¡the¡¡moisture¡¡in¡¡this¡¡process¡¡rises¡¡or¡¡falls¡£¡¡We



must¡¡think¡¡of¡¡it¡¡as¡¡a¡¡river¡¡flowing¡¡up¡¡and¡¡down¡¡in¡¡a¡¡circle¡¡and¡¡made



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and¡¡the¡¡order¡¡of¡¡sequence£»¡¡at¡¡all¡¡events£»¡¡in¡¡this¡¡process¡¡always



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about¡¡the¡¡earth¡£



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earth¡¡again¡¡when¡¡it¡¡gets¡¡cold¡£¡¡These¡¡processes¡¡and£»¡¡in¡¡some¡¡cases£»



their¡¡varieties¡¡are¡¡distinguished¡¡by¡¡special¡¡names¡£¡¡When¡¡the¡¡water



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it¡¡is¡¡rain¡£







¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡10







¡¡¡¡Some¡¡of¡¡the¡¡vapour¡¡that¡¡is¡¡formed¡¡by¡¡day¡¡does¡¡not¡¡rise¡¡high



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is¡¡being¡¡raised¡¡is¡¡small¡£¡¡When¡¡this¡¡cools¡¡and¡¡descends¡¡at¡¡night¡¡it



is¡¡called¡¡dew¡¡and¡¡hoar¡­frost¡£¡¡When¡¡the¡¡vapour¡¡is¡¡frozen¡¡before¡¡it



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moisture¡¡that¡¡has¡¡been¡¡raised¡¡nor¡¡the¡¡cold¡¡sufficient¡¡£¨owing¡¡to¡¡the



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prove¡¡that¡¡these¡¡phenomena¡¡occur¡¡because¡¡the¡¡vapour¡¡does¡¡not¡¡rise



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which¡¡explains¡¡why¡¡dew¡¡is¡¡found¡¡in¡¡warm¡¡weather¡¡and¡¡not¡¡in¡¡cold¡£¡¡For



the¡¡south¡¡wind¡¡brings¡¡warm£»¡¡and¡¡the¡¡north£»¡¡wintry¡¡weather¡£¡¡For¡¡the



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heat¡¡by¡¡a¡¡sort¡¡of¡¡recoil£»¡¡so¡¡that¡¡there¡¡is¡¡more¡¡evaporation¡¡and¡¡not



less¡£¡¡This¡¡is¡¡a¡¡thing¡¡which¡¡we¡¡can¡¡often¡¡observe¡¡in¡¡other¡¡places



too¡£¡¡Wells£»¡¡for¡¡instance£»¡¡give¡¡off¡¡more¡¡vapour¡¡in¡¡a¡¡north¡¡than¡¡in¡¡a



south¡¡wind¡£¡¡Only¡¡the¡¡north¡¡winds¡¡quench¡¡the¡¡heat¡¡before¡¡any



considerable¡¡quantity¡¡of¡¡vapour¡¡has¡¡gathered£»¡¡while¡¡in¡¡a¡¡south¡¡wind



the¡¡evaporation¡¡is¡¡allowed¡¡to¡¡accumulate¡£



¡¡¡¡Water£»¡¡once¡¡formed£»¡¡does¡¡not¡¡freeze¡¡on¡¡the¡¡surface¡¡of¡¡the¡¡earth£»



in¡¡the¡¡way¡¡that¡¡it¡¡does¡¡in¡¡the¡¡region¡¡of¡¡the¡¡clouds¡£







¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡11







¡¡¡¡From¡¡the¡¡latter¡¡there¡¡fall¡¡three¡¡bodies¡¡condensed¡¡by¡¡cold£»¡¡namely



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lower¡¡level¡¡and¡¡are¡¡due¡¡to¡¡the¡¡same¡¡causes£»¡¡differing¡¡from¡¡them¡¡only



in¡¡degree¡¡and¡¡quantity¡£



¡¡¡¡Snow¡¡and¡¡hoar¡­frost¡¡are¡¡one¡¡and¡¡the¡¡same¡¡thing£»¡¡and¡¡so¡¡are¡¡rain



and¡¡dew£º¡¡only¡¡there¡¡is¡¡a¡¡great¡¡deal¡¡of¡¡the¡¡former¡¡and¡¡little¡¡of¡¡the



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for¡¡the¡¡region¡¡from¡¡which¡¡and¡¡the¡¡time¡¡during¡¡which¡¡the¡¡vapour¡¡is



collected¡¡are¡¡considerable¡£¡¡But¡¡of¡¡dew¡¡there¡¡is¡¡little£º¡¡for¡¡the¡¡vapo

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