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¡¡as¡¡the¡¡square¡¡of¡¡the¡¡distance£¿¡¡That¡¡was¡¡the¡¡tangible¡¡form¡¡in¡¡which¡¡the¡¡problem¡¡presented¡¡itself¡¡to¡¡Newton¡£¡¡The¡¡mathematical¡¡solution¡¡of¡¡the¡¡problem¡¡was¡¡simple¡¡enough¡£¡¡It¡¡is¡¡based¡¡on¡¡a¡¡comparison¡¡of¡¡the¡¡moon's¡¡distance¡¡with¡¡the¡¡length¡¡of¡¡the¡¡earth's¡¡radius¡£¡¡On¡¡making¡¡this¡¡calculation£»¡¡Newton¡¡found¡¡that¡¡the¡¡pull¡¡of¡¡gravitationif¡¡that¡¡were¡¡really¡¡the¡¡force¡¡that¡¡controls¡¡the¡¡moongives¡¡that¡¡body¡¡a¡¡fall¡¡of¡¡slightly¡¡over¡¡fifteen¡¡feet¡¡in¡¡the¡¡first¡¡minute£»¡¡instead¡¡of¡¡thirteen¡¡feet¡£¡¡Here¡¡was¡¡surely¡¡a¡¡suggestive¡¡approximation£»¡¡yet£»¡¡on¡¡the¡¡other¡¡band£»¡¡the¡¡discrepancy¡¡seemed¡¡to¡¡be¡¡too¡¡great¡¡to¡¡warrant¡¡him¡¡in¡¡the¡¡supposition¡¡that¡¡he¡¡had¡¡found¡¡the¡¡true¡¡solution¡£¡¡He¡¡therefore¡¡dismissed¡¡the¡¡matter¡¡from¡¡his¡¡mind¡¡for¡¡the¡¡time¡¡being£»¡¡nor¡¡did¡¡he¡¡return¡¡to¡¡it¡¡definitely¡¡for¡¡some¡¡years¡£¡¡£ûillustration¡¡caption¡¡=¡¡¡¡DIAGRAM¡¡TO¡¡ILLUSTRATE¡¡NEWTON'S¡¡LAW¡¡OF¡¡GRAVITATION¡¡£¨E¡¡represents¡¡the¡¡earth¡¡and¡¡A¡¡the¡¡moon¡£¡¡Were¡¡the¡¡earth's¡¡pull¡¡on¡¡the¡¡moon¡¡to¡¡cease£»¡¡the¡¡moon's¡¡inertia¡¡would¡¡cause¡¡it¡¡to¡¡take¡¡the¡¡tangential¡¡course£»¡¡AB¡£¡¡On¡¡the¡¡other¡¡hand£»¡¡were¡¡the¡¡moon's¡¡motion¡¡to¡¡be¡¡stopped¡¡for¡¡an¡¡instant£»¡¡the¡¡moon¡¡would¡¡fall¡¡directly¡¡towards¡¡the¡¡earth£»¡¡along¡¡the¡¡line¡¡AD¡£¡¡The¡¡moon's¡¡actual¡¡orbit£»¡¡resulting¡¡from¡¡these¡¡component¡¡forces£»¡¡is¡¡AC¡£¡¡Let¡¡AC¡¡represent¡¡the¡¡actual¡¡flight¡¡of¡¡the¡¡moon¡¡in¡¡one¡¡minute¡£¡¡Then¡¡BC£»¡¡which¡¡is¡¡obviously¡¡equal¡¡to¡¡AD£»¡¡represents¡¡the¡¡distance¡¡which¡¡the¡¡moon¡¡virtually¡¡falls¡¡towards¡¡the¡¡earth¡¡in¡¡one¡¡minute¡£¡¡Actual¡¡computation£»¡¡based¡¡on¡¡measurements¡¡of¡¡the¡¡moon's¡¡orbit£»¡¡showed¡¡this¡¡distance¡¡to¡¡be¡¡about¡¡fifteen¡¡feet¡£¡¡Another¡¡computation¡¡showed¡¡that¡¡this¡¡is¡¡the¡¡distance¡¡that¡¡the¡¡moon¡¡would¡¡fall¡¡towards¡¡the¡¡earth¡¡under¡¡the¡¡influence¡¡of¡¡gravity£»¡¡on¡¡the¡¡supposition¡¡that¡¡the¡¡force¡¡of¡¡gravity¡¡decreases¡¡inversely¡¡with¡¡the¡¡square¡¡of¡¡the¡¡distance£»¡¡the¡¡basis¡¡of¡¡comparison¡¡being¡¡furnished¡¡by¡¡falling¡¡bodies¡¡at¡¡the¡¡surface¡¡of¡¡the¡¡earth¡£¡¡Theory¡¡and¡¡observations¡¡thus¡¡coinciding£»¡¡Newton¡¡was¡¡justified¡¡in¡¡declaring¡¡that¡¡the¡¡force¡¡that¡¡pulls¡¡the¡¡moon¡¡towards¡¡the¡¡earth¡¡and¡¡keeps¡¡it¡¡in¡¡its¡¡orbit£»¡¡is¡¡the¡¡familiar¡¡force¡¡of¡¡gravity£»¡¡and¡¡that¡¡this¡¡varies¡¡inversely¡¡as¡¡the¡¡square¡¡of¡¡the¡¡distance¡££©£ý¡¡It¡¡was¡¡to¡¡appear¡¡in¡¡due¡¡time¡¡that¡¡Newton's¡¡hypothesis¡¡was¡¡perfectly¡¡valid¡¡and¡¡that¡¡his¡¡method¡¡of¡¡attempted¡¡demonstration¡¡was¡¡equally¡¡so¡£¡¡The¡¡difficulty¡¡was¡¡that¡¡the¡¡earth's¡¡proper¡¡dimensions¡¡were¡¡not¡¡at¡¡that¡¡time¡¡known¡£¡¡A¡¡wrong¡¡estimate¡¡of¡¡the¡¡earth's¡¡size¡¡vitiated¡¡all¡¡the¡¡other¡¡calculations¡¡involved£»¡¡since¡¡the¡¡measurement¡¡of¡¡the¡¡moon's¡¡distance¡¡depends¡¡upon¡¡the¡¡observation¡¡of¡¡the¡¡parallax£»¡¡which¡¡cannot¡¡lead¡¡to¡¡a¡¡correct¡¡computation¡¡unless¡¡the¡¡length¡¡of¡¡the¡¡earth's¡¡radius¡¡is¡¡accurately¡¡known¡£¡¡Newton's¡¡first¡¡calculation¡¡was¡¡made¡¡as¡¡early¡¡as¡¡1666£»¡¡and¡¡it¡¡was¡¡not¡¡until¡¡1682¡¡that¡¡his¡¡attention¡¡was¡¡called¡¡to¡¡a¡¡new¡¡and¡¡apparently¡¡accurate¡¡measurement¡¡of¡¡a¡¡degree¡¡of¡¡the¡¡earth's¡¡meridian¡¡made¡¡by¡¡the¡¡French¡¡astronomer¡¡Picard¡£¡¡The¡¡new¡¡measurement¡¡made¡¡a¡¡degree¡¡of¡¡the¡¡earth's¡¡surface¡¡69¡£10¡¡miles£»¡¡instead¡¡of¡¡sixty¡¡miles¡£¡¡Learning¡¡of¡¡this¡¡materially¡¡altered¡¡calculation¡¡as¡¡to¡¡the¡¡earth's¡¡size£»¡¡Newton¡¡was¡¡led¡¡to¡¡take¡¡up¡¡again¡¡his¡¡problem¡¡of¡¡the¡¡falling¡¡moon¡£¡¡As¡¡he¡¡proceeded¡¡with¡¡his¡¡computation£»¡¡it¡¡became¡¡more¡¡and¡¡more¡¡certain¡¡that¡¡this¡¡time¡¡the¡¡result¡¡was¡¡to¡¡harmonize¡¡with¡¡the¡¡observed¡¡facts¡£¡¡As¡¡the¡¡story¡¡goes£»¡¡he¡¡was¡¡so¡¡completely¡¡overwhelmed¡¡with¡¡emotion¡¡that¡¡he¡¡was¡¡forced¡¡to¡¡ask¡¡a¡¡friend¡¡to¡¡complete¡¡the¡¡simple¡¡calculation¡£¡¡That¡¡story¡¡may¡¡well¡¡be¡¡true£»¡¡for£»¡¡simple¡¡though¡¡the¡¡computation¡¡was£»¡¡its¡¡result¡¡was¡¡perhaps¡¡the¡¡most¡¡wonderful¡¡demonstration¡¡hitherto¡¡achieved¡¡in¡¡the¡¡entire¡¡field¡¡of¡¡science¡£¡¡Now¡¡at¡¡last¡¡it¡¡was¡¡known¡¡that¡¡the¡¡force¡¡of¡¡gravitation¡¡operates¡¡at¡¡the¡¡distance¡¡of¡¡the¡¡moon£»¡¡and¡¡holds¡¡that¡¡body¡¡in¡¡its¡¡elliptical¡¡orbit£»¡¡and¡¡it¡¡required¡¡but¡¡a¡¡slight¡¡effort¡¡of¡¡the¡¡imagination¡¡to¡¡assume¡¡that¡¡the¡¡force¡¡which¡¡operates¡¡through¡¡such¡¡a¡¡reach¡¡of¡¡space¡¡extends¡¡its¡¡influence¡¡yet¡¡more¡¡widely¡£¡¡That¡¡such¡¡is¡¡really¡¡the¡¡case¡¡was¡¡demonstrated¡¡presently¡¡through¡¡calculations¡¡as¡¡to¡¡the¡¡moons¡¡of¡¡Jupiter¡¡and¡¡by¡¡similar¡¡computations¡¡regarding¡¡the¡¡orbital¡¡motions¡¡of¡¡the¡¡various¡¡planets¡£¡¡All¡¡results¡¡harmonizing£»¡¡Newton¡¡was¡¡justified¡¡in¡¡reaching¡¡the¡¡conclusion¡¡that¡¡gravitation¡¡is¡¡a¡¡universal¡¡property¡¡of¡¡matter¡£¡¡It¡¡remained£»¡¡as¡¡we¡¡shall¡¡see£»¡¡for¡¡nineteenth¡­century¡¡scientists¡¡to¡¡prove¡¡that¡¡the¡¡same¡¡force¡¡actually¡¡operates¡¡up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