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f¡¡the¡¡moon£»¡¡and¡¡both¡¡sun¡¡and¡¡moon¡¡disturb¡¡our¡¡sea£»¡¡as¡¡we¡¡shall¡¡hereafter¡¡explain¡£¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¨SCHOLIUM¡¡¡¨The¡¡force¡¡which¡¡retains¡¡the¡¡celestial¡¡bodies¡¡in¡¡their¡¡orbits¡¡has¡¡been¡¡hitherto¡¡called¡¡centripetal¡¡force£»¡¡but¡¡it¡¡being¡¡now¡¡made¡¡plain¡¡that¡¡it¡¡can¡¡be¡¡no¡¡other¡¡than¡¡a¡¡gravitating¡¡force£»¡¡we¡¡shall¡¡hereafter¡¡call¡¡it¡¡gravity¡£¡¡For¡¡the¡¡cause¡¡of¡¡the¡¡centripetal¡¡force¡¡which¡¡retains¡¡the¡¡moon¡¡in¡¡its¡¡orbit¡¡will¡¡extend¡¡itself¡¡to¡¡all¡¡the¡¡planets¡¡by¡¡Rules¡¡i¡££»¡¡ii¡££»¡¡and¡¡iii¡£¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¨PROPOSITION¡¡VI¡££»¡¡THEOREM¡¡VI¡£¡¡¡¨That¡¡all¡¡bodies¡¡gravitate¡¡towards¡¡every¡¡planet£»¡¡and¡¡that¡¡the¡¡weights¡¡of¡¡the¡¡bodies¡¡towards¡¡any¡¡the¡¡same¡¡planet£»¡¡at¡¡equal¡¡distances¡¡from¡¡the¡¡centre¡¡of¡¡the¡¡planet£»¡¡are¡¡proportional¡¡to¡¡the¡¡quantities¡¡of¡¡matter¡¡which¡¡they¡¡severally¡¡contain¡£
¡¨It¡¡has¡¡been¡¡now¡¡a¡¡long¡¡time¡¡observed¡¡by¡¡others¡¡that¡¡all¡¡sorts¡¡of¡¡heavy¡¡bodies¡¡£¨allowance¡¡being¡¡made¡¡for¡¡the¡¡inability¡¡of¡¡retardation¡¡which¡¡they¡¡suffer¡¡from¡¡a¡¡small¡¡power¡¡of¡¡resistance¡¡in¡¡the¡¡air£©¡¡descend¡¡to¡¡the¡¡earth¡¡FROM¡¡EQUAL¡¡HEIGHTS¡¡in¡¡equal¡¡times£»¡¡and¡¡that¡¡equality¡¡of¡¡times¡¡we¡¡may¡¡distinguish¡¡to¡¡a¡¡great¡¡accuracy¡¡by¡¡help¡¡of¡¡pendulums¡£¡¡I¡¡tried¡¡the¡¡thing¡¡in¡¡gold£»¡¡silver£»¡¡lead£»¡¡glass£»¡¡sand£»¡¡common¡¡salt£»¡¡wood£»¡¡water£»¡¡and¡¡wheat¡£¡¡I¡¡provided¡¡two¡¡wooden¡¡boxes£»¡¡round¡¡and¡¡equal£º¡¡I¡¡filled¡¡the¡¡one¡¡with¡¡wood£»¡¡and¡¡suspended¡¡an¡¡equal¡¡weight¡¡of¡¡gold¡¡£¨as¡¡exactly¡¡as¡¡I¡¡could£©¡¡in¡¡the¡¡centre¡¡of¡¡oscillation¡¡of¡¡the¡¡other¡£¡¡The¡¡boxes¡¡hanging¡¡by¡¡eleven¡¡feet£»¡¡made¡¡a¡¡couple¡¡of¡¡pendulums¡¡exactly¡¡equal¡¡in¡¡weight¡¡and¡¡figure£»¡¡and¡¡equally¡¡receiving¡¡the¡¡resistance¡¡of¡¡the¡¡air¡£¡¡And£»¡¡placing¡¡the¡¡one¡¡by¡¡the¡¡other£»¡¡I¡¡observed¡¡them¡¡to¡¡play¡¡together¡¡forward¡¡and¡¡backward£»¡¡for¡¡a¡¡long¡¡time£»¡¡with¡¡equal¡¡vibrations¡£¡¡And¡¡therefore¡¡the¡¡quantity¡¡of¡¡matter¡¡in¡¡gold¡¡was¡¡to¡¡the¡¡quantity¡¡of¡¡matter¡¡in¡¡the¡¡wood¡¡as¡¡the¡¡action¡¡of¡¡the¡¡motive¡¡force¡¡£¨or¡¡vis¡¡motrix£©¡¡upon¡¡all¡¡the¡¡gold¡¡to¡¡the¡¡action¡¡of¡¡the¡¡same¡¡upon¡¡all¡¡the¡¡woodthat¡¡is£»¡¡as¡¡the¡¡weight¡¡of¡¡the¡¡one¡¡to¡¡the¡¡weight¡¡of¡¡the¡¡other£º¡¡and¡¡the¡¡like¡¡happened¡¡in¡¡the¡¡other¡¡bodies¡£¡¡By¡¡these¡¡experiments£»¡¡in¡¡bodies¡¡of¡¡the¡¡same¡¡weight£»¡¡I¡¡could¡¡manifestly¡¡have¡¡discovered¡¡a¡¡difference¡¡of¡¡matter¡¡less¡¡than¡¡the¡¡thousandth¡¡part¡¡of¡¡the¡¡whole£»¡¡had¡¡any¡¡such¡¡been¡£¡¡But£»¡¡without¡¡all¡¡doubt£»¡¡the¡¡nature¡¡of¡¡gravity¡¡towards¡¡the¡¡planets¡¡is¡¡the¡¡same¡¡as¡¡towards¡¡the¡¡earth¡£¡¡For£»¡¡should¡¡we¡¡imagine¡¡our¡¡terrestrial¡¡bodies¡¡removed¡¡to¡¡the¡¡orb¡¡of¡¡the¡¡moon£»¡¡and¡¡there£»¡¡together¡¡with¡¡the¡¡moon£»¡¡deprived¡¡of¡¡all¡¡motion£»¡¡to¡¡be¡¡let¡¡go£»¡¡so¡¡as¡¡to¡¡fall¡¡together¡¡towards¡¡the¡¡earth£»¡¡it¡¡is¡¡certain£»¡¡from¡¡what¡¡we¡¡have¡¡demonstrated¡¡before£»¡¡that£»¡¡in¡¡equal¡¡times£»¡¡they¡¡would¡¡describe¡¡equal¡¡spaces¡¡with¡¡the¡¡moon£»¡¡and¡¡of¡¡consequence¡¡are¡¡to¡¡the¡¡moon£»¡¡in¡¡quantity¡¡and¡¡matter£»¡¡as¡¡their¡¡weights¡¡to¡¡its¡¡weight¡£¡¡¡¨Moreover£»¡¡since¡¡the¡¡satellites¡¡of¡¡Jupiter¡¡perform¡¡their¡¡revolutions¡¡in¡¡times¡¡which¡¡observe¡¡the¡¡sesquiplicate¡¡proportion¡¡of¡¡their¡¡distances¡¡from¡¡Jupiter's¡¡centre£»¡¡their¡¡accelerative¡¡gravities¡¡towards¡¡Jupiter¡¡will¡¡be¡¡reciprocally¡¡as¡¡the¡¡square¡¡of¡¡their¡¡distances¡¡from¡¡Jupiter's¡¡centrethat¡¡is£»¡¡equal£»¡¡at¡¡equal¡¡distances¡£¡¡And£»¡¡therefore£»¡¡these¡¡satellites£»¡¡if¡¡supposed¡¡to¡¡fall¡¡TOWARDS¡¡JUPITER¡¡from¡¡equal¡¡heights£»¡¡would¡¡describe¡¡equal¡¡spaces¡¡in¡¡equal¡¡times£»¡¡in¡¡like¡¡manner¡¡as¡¡heavy¡¡bodies¡¡do¡¡on¡¡our¡¡earth¡£¡¡And£»¡¡by¡¡the¡¡same¡¡argument£»¡¡if¡¡the¡¡circumsolar¡¡planets¡¡were¡¡supposed¡¡to¡¡be¡¡let¡¡fall¡¡at¡¡equal¡¡distances¡¡from¡¡the¡¡sun£»¡¡they¡¡would£»¡¡in¡¡their¡¡descent¡¡towards¡¡the¡¡sun£»¡¡describe¡¡equal¡¡spaces¡¡in¡¡equal¡¡times¡£¡¡But¡¡forces¡¡which¡¡equally¡¡accelerate¡¡unequal¡¡bodies¡¡must¡¡be¡¡as¡¡those¡¡bodiesthat¡¡is¡¡to¡¡say£»¡¡the¡¡weights¡¡of¡¡the¡¡planets¡¡£¨TOWARDS¡¡THE¡¡SUN¡¡must¡¡be¡¡as¡¡their¡¡quantities¡¡of¡¡matter¡£¡¡Further£»¡¡that¡¡the¡¡weights¡¡of¡¡Jupiter¡¡and¡¡his¡¡satellites¡¡towards¡¡the¡¡sun¡¡are¡¡proportional¡¡to¡¡the¡¡several¡¡quantities¡¡of¡¡their¡¡matter£»¡¡appears¡¡from¡¡the¡¡exceedingly¡¡regular¡¡motions¡¡of¡¡the¡¡satellites¡£¡¡For¡¡if¡¡some¡¡of¡¡these¡¡bodies¡¡were¡¡more¡¡strongly¡¡attracted¡¡to¡¡the¡¡sun¡¡in¡¡proportion¡¡to¡¡their¡¡quantity¡¡of¡¡matter¡¡than¡¡others£»¡¡the¡¡motions¡¡of¡¡the¡¡satellites¡¡would¡¡be¡¡disturbed¡¡by¡¡that¡¡inequality¡¡of¡¡attraction¡£¡¡If¡¡at¡¡equal¡¡distances¡¡from¡¡the¡¡sun¡¡any¡¡satellite£»¡¡in¡¡proportion¡¡to¡¡the¡¡quantity¡¡of¡¡its¡¡matter£»¡¡did¡¡gravitate¡¡towards¡¡the¡¡sun¡¡with¡¡a¡¡force¡¡greater¡¡than¡¡Jupiter¡¡in¡¡proportion¡¡to¡¡his£»¡¡according¡¡to¡¡any¡¡given¡¡proportion£»¡¡suppose¡¡d¡¡to¡¡e£»¡¡then¡¡the¡¡distance¡¡between¡¡the¡¡centres¡¡of¡¡the¡¡sun¡¡and¡¡of¡¡the¡¡satellite's¡¡orbit¡¡would¡¡be¡¡always¡¡greater¡¡than¡¡the¡¡distance¡¡between¡¡the¡¡centres¡¡of¡¡the¡¡sun¡¡and¡¡of¡¡Jupiter¡¡nearly¡¡in¡¡the¡¡subduplicate¡¡of¡¡that¡¡proportion£º¡¡as¡¡by¡¡some¡¡computations¡¡I¡¡have¡¡found¡£¡¡And¡¡if¡¡the¡¡satellite¡¡did¡¡gravitate¡¡towards¡¡the¡¡sun¡¡with¡¡a¡¡force£»¡¡lesser¡¡in¡¡the¡¡proportion¡¡of¡¡e¡¡to¡¡d£»¡¡the¡¡distance¡¡of¡¡the¡¡centre¡¡of¡¡the¡¡satellite's¡¡orb¡¡from¡¡the¡¡sun¡¡would¡¡be¡¡less¡¡than¡¡the¡¡distance¡¡of¡¡the¡¡centre¡¡of¡¡Jupiter¡¡from¡¡the¡¡sun¡¡in¡¡the¡¡subduplicate¡¡of¡¡the¡¡same¡¡proportion¡£¡¡Therefore£»¡¡if¡¡at¡¡equal¡¡distances¡¡from¡¡the¡¡sun£»¡¡the¡¡accelerative¡¡gravity¡¡of¡¡any¡¡satellite¡¡towards¡¡the¡¡sun¡¡were¡¡greater¡¡or¡¡less¡¡than¡¡the¡¡accelerative¡¡gravity¡¡of¡¡Jupiter¡¡towards¡¡the¡¡sun¡¡by¡¡one¡one¡thousandth¡¡part¡¡of¡¡the¡¡whole¡¡gravity£»¡¡the¡¡distance¡¡of¡¡the¡¡centre¡¡of¡¡the¡¡satellite's¡¡orbit¡¡from¡¡the¡¡sun¡¡would¡¡be¡¡greater¡¡or¡¡less¡¡than¡¡the¡¡distance¡¡of¡¡Jupiter¡¡from¡¡the¡¡sun¡¡by¡¡one¡¡one¡two¡thousandth¡¡part¡¡of¡¡the¡¡whole¡¡distancethat¡¡is£»¡¡by¡¡a¡¡fifth¡¡part¡¡of¡¡the¡¡distance¡¡of¡¡the¡¡utmost¡¡satellite¡¡from¡¡the¡¡centre¡¡of¡¡Jupiter£»¡¡an¡¡eccentricity¡¡of¡¡the¡¡orbit¡¡which¡¡would¡¡be¡¡very¡¡sensible¡£¡¡But¡¡the¡¡orbits¡¡of¡¡the¡¡satellites¡¡are¡¡concentric¡¡to¡¡Jupiter£»¡¡and¡¡therefore¡¡the¡¡accelerative¡¡gravities¡¡of¡¡Jupiter¡¡and¡¡of¡¡all¡¡its¡¡satellites¡¡towards¡¡the¡¡sun£»¡¡at¡¡equal¡¡distances¡¡from¡¡the¡¡sun£»¡¡are¡¡as¡¡their¡¡several¡¡quantities¡¡of¡¡matter£»¡¡and¡¡the¡¡weights¡¡of¡¡the¡¡moon¡¡and¡¡of¡¡the¡¡earth¡¡towards¡¡the¡¡sun¡¡are¡¡either¡¡none£»¡¡or¡¡accurately¡¡proportional¡¡to¡¡the¡¡masses¡¡of¡¡matter¡¡which¡¡they¡¡contain¡£¡¡¡¨COR¡£¡¡5¡£The¡¡power¡¡of¡¡gravity¡¡is¡¡of¡¡a¡¡different¡¡nature¡¡from¡¡the¡¡power¡¡of¡¡magnetism£»¡¡for¡¡the¡¡magnetic¡¡attraction¡¡is¡¡not¡¡as¡¡the¡¡matter¡¡attracted¡£¡¡Some¡¡bodies¡¡are¡¡attracted¡¡more¡¡by¡¡the¡¡magnet£»¡¡others¡¡less£»¡¡most¡¡bodies¡¡not¡¡at¡¡all¡£¡¡The¡¡power¡¡of¡¡magnetism¡¡in¡¡one¡¡and¡¡the¡¡same¡¡body¡¡may¡¡be¡¡increased¡¡and¡¡diminished£»¡¡and¡¡is¡¡sometimes¡¡far¡¡stronger£»¡¡for¡¡the¡¡quantity¡¡of¡¡matter£»¡¡than¡¡the¡¡power¡¡of¡¡gravity£»¡¡and¡¡in¡¡receding¡¡from¡¡the¡¡magnet¡¡decreases¡¡not¡¡in¡¡the¡¡duplicate£»¡¡but¡¡almost¡¡in¡¡the¡¡triplicate¡¡proportion¡¡of¡¡the¡¡distance£»¡¡as¡¡nearly¡¡as¡¡I¡¡could¡¡judge¡¡from¡¡some¡¡rude¡¡observations¡£
¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¡¨PROPOSITION¡¡VII¡££»¡¡THEOREM¡¡VII¡£¡¡¡¨That¡¡there¡¡is¡¡a¡¡power¡¡of¡¡gravity¡¡tending¡¡to¡¡all¡¡bodies£»¡¡proportional¡¡to¡¡the¡¡several¡¡quantities¡¡of¡¡matter¡¡which¡¡they¡¡contain¡£
That¡¡all¡¡the¡¡planets¡¡mutually¡¡gravitate¡¡one¡¡towards¡¡another¡¡we¡¡have¡¡proved¡¡before£»¡¡as¡¡well¡¡as¡¡that¡¡the¡¡force¡¡of¡¡gravity¡¡towards¡¡every¡¡one¡¡of¡¡them¡¡considered¡¡apart£»¡¡is¡¡reciprocally¡¡as¡¡the¡¡square¡¡of¡¡the¡¡distance¡¡of¡¡places¡¡from¡¡the¡¡centre¡¡of¡¡the¡¡planet¡£¡¡And¡¡thence¡¡it¡¡follows£»¡¡that¡¡the¡¡gravity¡¡tending¡¡towards¡¡all¡¡the¡¡planets¡¡is¡¡proportional¡¡to¡¡the¡¡matter¡¡which¡¡they¡¡contain¡£¡¡¡¨Moreover£»¡¡since¡¡all¡¡the¡¡parts¡¡of¡¡any¡¡planet¡¡A¡¡gravitates¡¡towards¡¡any¡¡other¡¡planet¡¡B£»¡¡and¡¡the¡¡gravity¡¡of¡¡every¡¡part¡¡is¡¡to¡¡the¡¡gravity¡¡of¡¡the¡¡whole¡¡as¡¡the¡¡matter¡¡of¡¡the¡¡part¡¡is¡¡to¡¡the¡¡matter¡¡of¡¡the¡¡whole£»¡¡and¡¡to¡¡every¡¡action¡¡corresponds¡¡a¡¡reaction£»¡¡therefore¡¡the¡¡planet¡¡B¡¡will£»¡¡on¡¡the¡¡other¡¡hand£»¡¡gravitate¡¡towards¡¡all¡¡the¡¡parts¡¡of¡¡planet¡¡A£»¡¡and¡¡its¡¡gravity¡¡towards¡¡any¡¡one¡¡part¡¡will¡¡be¡¡to¡¡the¡¡gravity¡¡towards¡¡the¡¡whole¡¡as¡¡the¡¡matter¡¡of¡¡the¡¡part¡¡to¡¡the¡¡matter¡¡of¡¡the¡¡whole¡£¡¡Q¡£E¡£D¡£
¡¨HENCE¡¡IT¡¡WOULD¡¡APPEAR¡¡THAT¡¡the¡¡force¡¡of¡¡the¡¡whole¡¡must¡¡arise¡¡from¡¡the¡¡force¡¡of¡¡the¡¡component¡¡parts¡£¡¨
Newton¡¡closes¡¡this¡¡remarkable¡¡Book¡¡iii¡£¡¡with¡¡the¡¡following¡¡words£º¡¡¡¨Hitherto¡¡we¡¡have¡¡explained¡¡the¡¡phenomena¡¡of¡¡the¡¡heavens¡¡and¡¡of¡¡our¡¡sea¡¡by¡¡the¡¡power¡¡of¡¡gravity£»¡¡but¡¡have¡¡not¡¡yet¡¡assigned¡¡the¡¡cause¡¡of¡¡this¡¡power¡£¡¡This¡¡is¡¡certain£»¡¡that¡¡it¡¡must¡¡proceed¡¡from¡¡a¡¡cause¡¡that¡¡penetrates¡¡to¡¡the¡¡very¡¡centre¡¡of¡¡the¡¡sun¡¡and¡¡planets£»¡¡without¡¡suffering¡¡the¡¡least¡¡diminution¡¡of¡¡its¡¡force£»¡¡that¡¡operates¡¡not¡¡according¡¡to¡¡the¡¡quantity¡¡of¡¡the¡¡surfaces¡¡of¡¡the¡¡particles¡¡upon¡¡which¡¡it¡¡acts¡¡£¨as¡¡mechanical¡¡causes¡¡used¡¡to¡¡do£©£»¡¡but¡¡according¡¡to¡¡the¡¡quantity¡¡of¡¡solid¡¡matter¡¡which¡¡they¡¡contain£»¡¡and¡¡propagates¡¡its¡¡virtue¡¡on¡¡all¡¡sides¡¡to¡¡immense¡¡distances£»¡¡decreasing¡¡always¡¡in¡¡the¡¡duplicate¡¡proportions¡¡of¡¡the¡¡distances¡£¡¡Gravitation¡¡towards¡¡the¡¡sun¡¡is¡¡made¡¡up¡¡out¡¡of¡¡the¡¡gravitations¡¡towards¡¡the¡¡several¡¡particles¡¡of¡¡which¡¡the¡¡body¡¡of¡¡the¡¡sun¡¡is¡¡composed£»¡¡and¡¡in¡¡receding¡¡from¡¡the¡¡sun¡¡decreases¡¡accurately¡¡in¡¡the¡¡duplicate¡¡proportion¡¡of¡¡the¡¡distances¡¡as¡¡far¡¡as¡¡the¡¡orb¡¡of¡¡Saturn£»¡¡as¡¡evidently¡¡appears¡¡from¡¡the¡¡quiescence¡¡of¡¡the¡¡aphelions¡¡of¡¡the¡¡planets£»¡¡nay£»¡¡and¡¡even¡¡to¡¡the¡¡remotest¡¡aphelions¡¡of¡¡the¡¡comets£»¡¡if¡¡those¡¡aphelions¡¡are¡¡also¡¡quiescent¡£¡¡But¡¡hitherto¡¡I¡¡have¡¡not¡¡been¡¡able¡¡to¡¡discover¡¡the¡¡cause¡¡of¡¡those¡¡properties¡¡of¡¡gravity¡¡from¡¡phenomena£»¡¡and¡¡I¡¡frame¡¡no¡¡hypothesis£»¡¡for¡¡whatever¡¡is¡¡not¡¡deduced¡¡from¡¡the¡¡phenomena¡¡is¡¡to¡¡be¡¡called¡¡an¡¡hypothesis£»¡¡and¡¡hypotheses£»¡¡whether¡¡metaphysical¡¡or¡¡physical£»¡¡whether¡¡of¡¡occult¡¡qualities¡¡or¡¡mechanical£»¡¡have¡¡no¡¡place¡¡in¡¡experimental¡¡philosophy¡£¡¡¡£¡¡¡£¡¡¡£¡¡And¡¡to¡¡us¡¡it¡¡is¡¡enough¡¡that¡¡gravity¡¡does¡¡really¡¡exist£»¡¡and¡¡act¡¡according¡¡to¡¡the¡¡laws¡¡which¡¡we¡¡have¡¡explained£»¡¡and¡¡abundantly¡¡serves¡¡to¡¡account¡¡for¡¡all¡¡the¡¡motions¡¡of¡¡the¡¡celestial¡¡bodies¡¡and¡¡of¡¡our¡¡sea¡£¡¨£§2£§
The¡¡very¡¡magnitude¡¡of¡¡the¡¡importance¡¡of¡¡the¡¡theory¡¡of¡¡universal¡¡gravitation¡¡made¡¡its¡¡general¡¡acceptance¡¡a¡¡matter¡¡of¡¡considerable¡¡time¡¡after¡¡the¡¡actual¡¡discovery¡£¡¡This¡¡opposition¡¡had¡¡of¡¡course¡¡been¡¡foreseen¡¡by¡¡Newton£»¡¡and£»¡¡much¡¡as¡¡be¡¡dreaded¡¡controversy£»¡¡he¡¡was¡¡prepared¡¡to¡¡face¡¡it¡¡and¡¡combat¡¡it¡¡to¡¡the¡¡bitter¡¡end¡£¡¡He¡¡knew¡¡that¡¡his¡¡theory¡¡was¡¡right£»¡¡it¡¡remained¡¡for¡¡him¡¡to¡¡convince¡¡the¡¡world¡¡of¡¡its¡¡truth¡£¡¡He¡¡knew¡¡that¡¡some¡¡of¡¡his¡¡contemporary¡¡philosophers¡¡would¡¡accept¡¡it¡¡at¡¡once£»¡¡others¡¡would¡¡at¡¡first¡¡doubt£»¡¡question£»¡¡and¡¡dispute£»¡¡but¡¡finally¡¡accept£»¡¡while¡¡still¡¡others¡¡would¡¡doubt¡¡and¡¡dispute¡¡until¡¡the¡¡end¡¡of¡¡their¡¡days¡£¡¡This¡¡had¡¡been¡¡the¡¡history¡¡of¡¡other¡¡great¡¡discoveries£»¡¡and¡¡this¡¡will¡¡probably¡¡be¡¡the¡¡history¡¡of¡¡most¡¡great¡¡discoveries¡¡for¡¡all¡¡time¡£¡¡But¡¡in¡¡this¡¡case¡¡the¡¡discoverer¡¡lived¡¡to¡¡see¡¡his¡¡theory¡¡accepted¡¡by¡¡practically¡¡all¡¡the¡¡great¡¡minds¡¡of¡¡his¡¡time¡£¡¡Delambre¡¡is¡¡authority¡¡for¡¡the¡¡following¡¡estimate¡¡of¡¡Newton¡¡by¡¡Lagrange¡£¡¡¡¨The¡¡celebrated¡¡Lagrange£»¡¨¡¡he¡¡says£»¡¡¡¨who¡¡frequently¡¡asserted¡¡that¡¡Newton¡¡was¡¡the¡¡greatest¡¡genius¡¡that¡¡ever¡¡existed£»¡¡used¡¡to¡¡add'and¡¡the¡¡most¡¡fortunate£»¡¡for¡¡we¡¡cannot¡¡find¡¡MORE¡¡THAN¡¡ONCE¡¡a¡¡system¡¡of¡¡the¡¡world¡¡to¡¡establish¡£'¡¡¡¨¡¡With¡¡pardonable¡¡exaggeration¡¡the¡¡admiring¡¡followers¡¡of¡¡the¡¡great¡¡generalizer¡¡pronounced¡¡this¡¡epitaph£º¡¡¡¡¡¨Nature¡¡and¡¡Nature's¡¡laws¡¡lay¡¡hid¡¡in¡¡night£»¡¡¡¡¡¡God¡¡said¡¡¡®Let¡¡Newton¡¡be£¡'¡¡and¡¡all¡¡was¡¡light¡£¡¨
XIII¡£¡¡INSTRUMENTS¡¡OF¡¡PRECISION¡¡IN¡¡THE¡¡AGE¡¡OF¡¡NEWTON¡¡During¡¡the¡¡Newtonian¡¡epoch¡¡there¡¡were¡¡numerous¡¡important¡¡inventions¡¡of¡¡scientific¡¡instruments£»¡¡as¡¡well¡¡as¡¡many¡¡improvements¡¡made¡¡upon¡¡the¡¡older¡¡ones¡£¡¡Some¡¡of¡¡these¡¡discoveries¡¡have¡¡been¡¡referred¡¡to¡¡briefly¡¡in¡¡other¡¡places£»¡¡but¡¡their¡¡importance¡¡in¡¡promoting¡¡scientific¡¡investigation¡¡warrants¡¡a¡¡fuller¡¡treatment¡¡of¡¡some¡¡of¡¡the¡¡more¡¡significant¡£¡¡Many¡¡of¡¡the¡¡errors¡¡that¡¡had¡¡arisen¡¡in¡¡various¡¡scientific¡¡calculations¡¡before¡¡the¡¡seventeenth¡¡century¡¡may¡¡be¡¡ascribed¡¡to¡¡the¡¡crudeness¡¡and¡¡inaccuracy¡¡in¡¡the¡¡construction¡¡of¡¡most¡¡scientific¡¡instruments¡£¡¡Scientists¡¡had¡¡not¡¡as¡¡yet¡¡learned¡¡that¡¡an¡¡approach¡¡to¡¡absolute¡¡accuracy¡¡was¡¡necessary¡¡in¡¡every¡¡investigation¡¡in¡¡the¡¡field¡¡of¡¡science£»¡¡and¡¡that¡¡such¡¡accuracy¡¡must¡¡be¡¡extended¡¡to¡¡the¡¡construction¡¡of¡¡the¡¡instruments¡¡used¡¡in¡¡these¡¡investigations¡¡and¡¡observations¡£¡¡In¡¡astronomy¡¡it¡¡is¡¡obvious¡¡that¡¡instruments¡¡of¡¡delicate¡¡exactness¡¡are¡¡most¡¡essential£»¡¡yet¡¡Tycho¡¡Brahe£»¡¡who¡¡lived¡¡in¡¡the¡¡sixteenth¡¡century£»¡¡is¡¡credited¡¡w