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their¡¡origin¡¡is¡¡plainly¡¡due¡¡to¡¡the¡¡plentiful¡¡supply¡¡of¡¡that¡¡secretion¡£



Hence¡¡the¡¡air¡¡is¡¡necessarily¡¡drier¡¡and¡¡the¡¡moist¡¡evaporation¡¡is¡¡so



dissolved¡¡and¡¡dissipated¡¡by¡¡the¡¡quantity¡¡of¡¡the¡¡hot¡¡exhalation¡¡as



not¡¡readily¡¡to¡¡condense¡¡into¡¡water¡£¡­But¡¡this¡¡phenomenon¡¡too¡¡shall¡¡be



explained¡¡more¡¡clearly¡¡later¡¡when¡¡the¡¡time¡¡comes¡¡to¡¡speak¡¡of¡¡the



winds¡£¡­So¡¡when¡¡there¡¡are¡¡many¡¡comets¡¡and¡¡they¡¡are¡¡dense£»¡¡it¡¡is¡¡as¡¡we



say£»¡¡and¡¡the¡¡years¡¡are¡¡clearly¡¡dry¡¡and¡¡windy¡£¡¡When¡¡they¡¡are¡¡fewer



and¡¡fainter¡¡this¡¡effect¡¡does¡¡not¡¡appear¡¡in¡¡the¡¡same¡¡degree£»¡¡though



as¡¡a¡¡rule¡¡the¡¡is¡¡found¡¡to¡¡be¡¡excessive¡¡either¡¡in¡¡duration¡¡or¡¡strength¡£



For¡¡instance¡¡when¡¡the¡¡stone¡¡at¡¡Aegospotami¡¡fell¡¡out¡¡of¡¡the¡¡air¡­it



had¡¡been¡¡carried¡¡up¡¡by¡¡a¡¡wind¡¡and¡¡fell¡¡down¡¡in¡¡the¡¡daytime¡­then¡¡too



a¡¡comet¡¡happened¡¡to¡¡have¡¡appeared¡¡in¡¡the¡¡west¡£¡¡And¡¡at¡¡the¡¡time¡¡of



the¡¡great¡¡comet¡¡the¡¡winter¡¡was¡¡dry¡¡and¡¡north¡¡winds¡¡prevailed£»¡¡and



the¡¡wave¡¡was¡¡due¡¡to¡¡an¡¡opposition¡¡of¡¡winds¡£¡¡For¡¡in¡¡the¡¡gulf¡¡a¡¡north



wind¡¡blew¡¡and¡¡outside¡¡it¡¡a¡¡violent¡¡south¡¡wind¡£¡¡Again¡¡in¡¡the¡¡archonship



of¡¡Nicomachus¡¡a¡¡comet¡¡appeared¡¡for¡¡a¡¡few¡¡days¡¡about¡¡the¡¡equinoctial



circle¡¡£¨this¡¡one¡¡had¡¡not¡¡risen¡¡in¡¡the¡¡west£©£»¡¡and¡¡simultaneously¡¡with



it¡¡there¡¡happened¡¡the¡¡storm¡¡at¡¡Corinth¡£



¡¡¡¡That¡¡there¡¡are¡¡few¡¡comets¡¡and¡¡that¡¡they¡¡appear¡¡rarely¡¡and¡¡outside



the¡¡tropic¡¡circles¡¡more¡¡than¡¡within¡¡them¡¡is¡¡due¡¡to¡¡the¡¡motion¡¡of¡¡the



sun¡¡and¡¡the¡¡stars¡£¡¡For¡¡this¡¡motion¡¡does¡¡not¡¡only¡¡cause¡¡the¡¡hot



principle¡¡to¡¡be¡¡secreted¡¡but¡¡also¡¡dissolves¡¡it¡¡when¡¡it¡¡is¡¡gathering¡£



But¡¡the¡¡chief¡¡reason¡¡is¡¡that¡¡most¡¡of¡¡this¡¡stuff¡¡collects¡¡in¡¡the¡¡region



of¡¡the¡¡milky¡¡way¡£







¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡8







¡¡¡¡Let¡¡us¡¡now¡¡explain¡¡the¡¡origin£»¡¡cause£»¡¡and¡¡nature¡¡of¡¡the¡¡milky¡¡way¡£



And¡¡here¡¡too¡¡let¡¡us¡¡begin¡¡by¡¡discussing¡¡the¡¡statements¡¡of¡¡others¡¡on



the¡¡subject¡£



¡¡¡¡£¨1£©¡¡Of¡¡the¡¡so¡­called¡¡Pythagoreans¡¡some¡¡say¡¡that¡¡this¡¡is¡¡the¡¡path



of¡¡one¡¡of¡¡the¡¡stars¡¡that¡¡fell¡¡from¡¡heaven¡¡at¡¡the¡¡time¡¡of¡¡Phaethon's



downfall¡£¡¡Others¡¡say¡¡that¡¡the¡¡sun¡¡used¡¡once¡¡to¡¡move¡¡in¡¡this¡¡circle¡¡and



that¡¡this¡¡region¡¡was¡¡scorched¡¡or¡¡met¡¡with¡¡some¡¡other¡¡affection¡¡of¡¡this



kind£»¡¡because¡¡of¡¡the¡¡sun¡¡and¡¡its¡¡motion¡£



¡¡¡¡But¡¡it¡¡is¡¡absurd¡¡not¡¡to¡¡see¡¡that¡¡if¡¡this¡¡were¡¡the¡¡reason¡¡the



circle¡¡of¡¡the¡¡Zodiac¡¡ought¡¡to¡¡be¡¡affected¡¡in¡¡the¡¡same¡¡way£»¡¡and



indeed¡¡more¡¡so¡¡than¡¡that¡¡of¡¡the¡¡milky¡¡way£»¡¡since¡¡not¡¡the¡¡sun¡¡only



but¡¡all¡¡the¡¡planets¡¡move¡¡in¡¡it¡£¡¡We¡¡can¡¡see¡¡the¡¡whole¡¡of¡¡this¡¡circle



£¨half¡¡of¡¡it¡¡being¡¡visible¡¡at¡¡any¡¡time¡¡of¡¡the¡¡night£©£»¡¡but¡¡it¡¡shows¡¡no



signs¡¡of¡¡any¡¡such¡¡affection¡¡except¡¡where¡¡a¡¡part¡¡of¡¡it¡¡touches¡¡the



circle¡¡of¡¡the¡¡milky¡¡way¡£



¡¡¡¡£¨2£©¡¡Anaxagoras£»¡¡Democritus£»¡¡and¡¡their¡¡schools¡¡say¡¡that¡¡the¡¡milky¡¡way



is¡¡the¡¡light¡¡of¡¡certain¡¡stars¡£¡¡For£»¡¡they¡¡say£»¡¡when¡¡the¡¡sun¡¡passes



below¡¡the¡¡earth¡¡some¡¡of¡¡the¡¡stars¡¡are¡¡hidden¡¡from¡¡it¡£¡¡Now¡¡the¡¡light¡¡of



those¡¡on¡¡which¡¡the¡¡sun¡¡shines¡¡is¡¡invisible£»¡¡being¡¡obscured¡¡by¡¡the¡¡of



the¡¡sun¡£¡¡But¡¡the¡¡milky¡¡way¡¡is¡¡the¡¡peculiar¡¡light¡¡of¡¡those¡¡stars



which¡¡are¡¡shaded¡¡by¡¡the¡¡earth¡¡from¡¡the¡¡sun's¡¡rays¡£



¡¡¡¡This£»¡¡too£»¡¡is¡¡obviously¡¡impossible¡£¡¡The¡¡milky¡¡way¡¡is¡¡always



unchanged¡¡and¡¡among¡¡the¡¡same¡¡constellations¡¡£¨for¡¡it¡¡is¡¡clearly¡¡a



greatest¡¡circle£©£»¡¡whereas£»¡¡since¡¡the¡¡sun¡¡does¡¡not¡¡remain¡¡in¡¡the¡¡same



place£»¡¡what¡¡is¡¡hidden¡¡from¡¡it¡¡differs¡¡at¡¡different¡¡times¡£¡¡Consequently



with¡¡the¡¡change¡¡of¡¡the¡¡sun's¡¡position¡¡the¡¡milky¡¡way¡¡ought¡¡to¡¡change



its¡¡position¡¡too£º¡¡but¡¡we¡¡find¡¡that¡¡this¡¡does¡¡not¡¡happen¡£¡¡Besides£»¡¡if



astronomical¡¡demonstrations¡¡are¡¡correct¡¡and¡¡the¡¡size¡¡of¡¡the¡¡sun¡¡is



greater¡¡than¡¡that¡¡of¡¡the¡¡earth¡¡and¡¡the¡¡distance¡¡of¡¡the¡¡stars¡¡from



the¡¡earth¡¡many¡¡times¡¡greater¡¡than¡¡that¡¡of¡¡the¡¡sun¡¡£¨just¡¡as¡¡the¡¡sun



is¡¡further¡¡from¡¡the¡¡earth¡¡than¡¡the¡¡moon£©£»¡¡then¡¡the¡¡cone¡¡made¡¡by¡¡the



rays¡¡of¡¡the¡¡sun¡¡would¡¡terminate¡¡at¡¡no¡¡great¡¡distance¡¡from¡¡the¡¡earth£»



and¡¡the¡¡shadow¡¡of¡¡the¡¡earth¡¡£¨what¡¡we¡¡call¡¡night£©¡¡would¡¡not¡¡reach¡¡the



stars¡£¡¡On¡¡the¡¡contrary£»¡¡the¡¡sun¡¡shines¡¡on¡¡all¡¡the¡¡stars¡¡and¡¡the



earth¡¡screens¡¡none¡¡of¡¡them¡£



¡¡¡¡£¨3£©¡¡There¡¡is¡¡a¡¡third¡¡theory¡¡about¡¡the¡¡milky¡¡way¡£¡¡Some¡¡say¡¡that¡¡it¡¡is



a¡¡reflection¡¡of¡¡our¡¡sight¡¡to¡¡the¡¡sun£»¡¡just¡¡as¡¡they¡¡say¡¡that¡¡the



comet¡¡is¡£



¡¡¡¡But¡¡this¡¡too¡¡is¡¡impossible¡£¡¡For¡¡if¡¡the¡¡eye¡¡and¡¡the¡¡mirror¡¡and¡¡the



whole¡¡of¡¡the¡¡object¡¡were¡¡severally¡¡at¡¡rest£»¡¡then¡¡the¡¡same¡¡part¡¡of



the¡¡image¡¡would¡¡appear¡¡at¡¡the¡¡same¡¡point¡¡in¡¡the¡¡mirror¡£¡¡But¡¡if¡¡the



mirror¡¡and¡¡the¡¡object¡¡move£»¡¡keeping¡¡the¡¡same¡¡distance¡¡from¡¡the¡¡eye



which¡¡is¡¡at¡¡rest£»¡¡but¡¡at¡¡different¡¡rates¡¡of¡¡speed¡¡and¡¡so¡¡not¡¡always¡¡at



the¡¡same¡¡interval¡¡from¡¡one¡¡another£»¡¡then¡¡it¡¡is¡¡impossible¡¡for¡¡the¡¡same



image¡¡always¡¡to¡¡appear¡¡in¡¡the¡¡same¡¡part¡¡of¡¡the¡¡mirror¡£¡¡Now¡¡the



constellations¡¡included¡¡in¡¡the¡¡circle¡¡of¡¡the¡¡milky¡¡way¡¡move£»¡¡and¡¡so



does¡¡the¡¡sun£»¡¡the¡¡object¡¡to¡¡which¡¡our¡¡sight¡¡is¡¡reflected£»¡¡but¡¡we¡¡stand



still¡£¡¡And¡¡the¡¡distance¡¡of¡¡those¡¡two¡¡from¡¡us¡¡is¡¡constant¡¡and



uniform£»¡¡but¡¡their¡¡distance¡¡from¡¡one¡¡another¡¡varies¡£¡¡For¡¡the¡¡Dolphin



sometimes¡¡rises¡¡at¡¡midnight£»¡¡sometimes¡¡in¡¡the¡¡morning¡£¡¡But¡¡in¡¡each



case¡¡the¡¡same¡¡parts¡¡of¡¡the¡¡milky¡¡way¡¡are¡¡found¡¡near¡¡it¡£¡¡But¡¡if¡¡it¡¡were



a¡¡reflection¡¡and¡¡not¡¡a¡¡genuine¡¡affection¡¡of¡¡these¡¡this¡¡ought¡¡not¡¡to¡¡be



the¡¡case¡£



¡¡¡¡Again£»¡¡we¡¡can¡¡see¡¡the¡¡milky¡¡way¡¡reflected¡¡at¡¡night¡¡in¡¡water¡¡and



similar¡¡mirrors¡£¡¡But¡¡under¡¡these¡¡circumstances¡¡it¡¡is¡¡impossible¡¡for



our¡¡sight¡¡to¡¡be¡¡reflected¡¡to¡¡the¡¡sun¡£



¡¡¡¡These¡¡considerations¡¡show¡¡that¡¡the¡¡milky¡¡way¡¡is¡¡not¡¡the¡¡path¡¡of



one¡¡of¡¡the¡¡planets£»¡¡nor¡¡the¡¡light¡¡of¡¡imperceptible¡¡stars£»¡¡nor¡¡a



reflection¡£¡¡And¡¡those¡¡are¡¡the¡¡chief¡¡theories¡¡handed¡¡down¡¡by¡¡others



hitherto¡£



¡¡¡¡Let¡¡us¡¡recall¡¡our¡¡fundamental¡¡principle¡¡and¡¡then¡¡explain¡¡our



views¡£¡¡We¡¡have¡¡already¡¡laid¡¡down¡¡that¡¡the¡¡outermost¡¡part¡¡of¡¡what¡¡is



called¡¡the¡¡air¡¡is¡¡potentially¡¡fire¡¡and¡¡that¡¡therefore¡¡when¡¡the¡¡air



is¡¡dissolved¡¡by¡¡motion£»¡¡there¡¡is¡¡separated¡¡off¡¡a¡¡kind¡¡of¡¡matter¡­and¡¡of



this¡¡matter¡¡we¡¡assert¡¡that¡¡comets¡¡consist¡£¡¡We¡¡must¡¡suppose¡¡that¡¡what



happens¡¡is¡¡the¡¡same¡¡as¡¡in¡¡the¡¡case¡¡of¡¡the¡¡comets¡¡when¡¡the¡¡matter



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



planets£»¡¡and¡¡for¡¡this¡¡reason¡¡most¡¡comets¡¡are¡¡found¡¡outside¡¡the



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



greatest¡¡circle£»¡¡and¡¡its¡¡position¡¡is¡¡such¡¡that¡¡it¡¡extends¡¡far



outside¡¡the¡¡tropic¡¡circles¡£¡¡Besides¡¡the¡¡region¡¡is¡¡full¡¡of¡¡the



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



'scattered'¡¡stars¡¡£¨you¡¡have¡¡only¡¡to¡¡look¡¡to¡¡see¡¡this¡¡clearly£©¡£¡¡So



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



the¡¡light¡¡is¡¡the¡¡motion¡¡of¡¡the¡¡constellations¡¡and¡¡nothing¡¡else¡£¡¡For¡¡if



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



'scattered'¡¡stars¡¡it¡¡is¡¡not¡¡possible¡¡to¡¡set¡¡down¡¡in¡¡the¡¡same¡¡way¡¡on



the¡¡sphere¡¡because¡¡none¡¡of¡¡them¡¡have¡¡an¡¡evident¡¡permanent¡¡position£»



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



former¡¡case¡¡is¡¡an¡¡affection¡¡of¡¡a¡¡single¡¡star¡¡here¡¡forms¡¡in¡¡the¡¡same



way¡¡in¡¡relation¡¡to¡¡a¡¡whole¡¡circle¡£¡¡So¡¡if¡¡we¡¡are¡¡to¡¡define¡¡the¡¡milky



way¡¡we¡¡may¡¡call¡¡it¡¡'a¡¡fringe¡¡attaching¡¡to¡¡the¡¡greatest¡¡circle£»¡¡and¡¡due



to¡¡the¡¡matter¡¡secreted'¡£¡¡This£»¡¡as¡¡we¡¡said¡¡before£»¡¡explains¡¡why¡¡there



are¡¡few¡¡comets¡¡and¡¡why¡¡they¡¡appear¡¡rarely£»¡¡it¡¡is¡¡because¡¡at¡¡each



revolution¡¡of¡¡the¡¡heavens¡¡this¡¡matter¡¡has¡¡always¡¡been¡¡and¡¡is¡¡always



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



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



terrestrial¡¡world¡¡which¡¡is¡¡continuous¡¡with¡¡the¡¡motions¡¡of¡¡the¡¡heavens£»



namely£»¡¡shooting¡­stars¡¡and¡¡the¡¡burning¡¡flame£»¡¡comets¡¡and¡¡the¡¡milky



way£»¡¡these¡¡being¡¡the¡¡chief¡¡affections¡¡that¡¡appear¡¡in¡¡that¡¡region¡£







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







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



after¡¡this¡¡and¡¡which¡¡immediately¡¡surrounds¡¡the¡¡earth¡£¡¡It¡¡is¡¡the¡¡region



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



of¡¡water¡¡above¡¡take¡¡place¡¡in¡¡it¡£¡¡We¡¡must¡¡consider¡¡the¡¡principles¡¡and



causes¡¡of¡¡all¡¡these¡¡phenomena¡¡too¡¡as¡¡before¡£¡¡The¡¡efficient¡¡and¡¡chief



and¡¡first¡¡cause¡¡is¡¡the¡¡circle¡¡in¡¡which¡¡the¡¡sun¡¡moves¡£¡¡For¡¡the¡¡sun¡¡as



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



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



the¡¡earth¡¡remains¡¡but¡¡the¡¡moisture¡¡surrounding¡¡it¡¡is¡¡made¡¡to¡¡evaporate



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