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¡¡observed¡¡that¡¡his¡¡pendulum¡¡might¡¡be¡¡constructed¡¡of¡¡any¡¡weight¡¡sufficiently¡¡heavy¡¡readily¡¡to¡¡overcome¡¡the¡¡atmospheric¡¡resistance£»¡¡and¡¡that£»¡¡with¡¡this¡¡qualification£»¡¡neither¡¡the¡¡weight¡¡nor¡¡the¡¡material¡¡had¡¡any¡¡influence¡¡upon¡¡the¡¡time¡¡of¡¡oscillation£»¡¡this¡¡being¡¡solely¡¡determined¡¡by¡¡the¡¡length¡¡of¡¡the¡¡cord¡£¡¡Naturally£»¡¡the¡¡practical¡¡utility¡¡of¡¡these¡¡discoveries¡¡was¡¡not¡¡overlooked¡¡by¡¡Galileo¡£¡¡Since¡¡a¡¡pendulum¡¡of¡¡a¡¡given¡¡length¡¡oscillates¡¡with¡¡unvarying¡¡rapidity£»¡¡here¡¡is¡¡an¡¡obvious¡¡means¡¡of¡¡measuring¡¡time¡£¡¡Galileo£»¡¡however£»¡¡appears¡¡not¡¡to¡¡have¡¡met¡¡with¡¡any¡¡great¡¡measure¡¡of¡¡success¡¡in¡¡putting¡¡this¡¡idea¡¡into¡¡practice¡£¡¡It¡¡remained¡¡for¡¡the¡¡mechanical¡¡ingenuity¡¡of¡¡Huyghens¡¡to¡¡construct¡¡a¡¡satisfactory¡¡pendulum¡¡clock¡£¡¡As¡¡a¡¡theoretical¡¡result¡¡of¡¡the¡¡studies¡¡of¡¡rolling¡¡and¡¡oscillating¡¡bodies£»¡¡there¡¡was¡¡developed¡¡what¡¡is¡¡usually¡¡spoken¡¡of¡¡as¡¡the¡¡third¡¡law¡¡of¡¡motionnamely£»¡¡the¡¡law¡¡that¡¡a¡¡given¡¡force¡¡operates¡¡upon¡¡a¡¡moving¡¡body¡¡with¡¡an¡¡effect¡¡proportionate¡¡to¡¡its¡¡effect¡¡upon¡¡the¡¡same¡¡body¡¡when¡¡at¡¡rest¡£¡¡Or£»¡¡as¡¡Whewell¡¡states¡¡the¡¡law£º¡¡¡¨The¡¡dynamical¡¡effect¡¡of¡¡force¡¡is¡¡as¡¡the¡¡statical¡¡effect£»¡¡that¡¡is£»¡¡the¡¡velocity¡¡which¡¡any¡¡force¡¡generates¡¡in¡¡a¡¡given¡¡time£»¡¡when¡¡it¡¡puts¡¡the¡¡body¡¡in¡¡motion£»¡¡is¡¡proportional¡¡to¡¡the¡¡pressure¡¡which¡¡this¡¡same¡¡force¡¡produces¡¡in¡¡a¡¡body¡¡at¡¡rest¡£¡¨£§2£§¡¡According¡¡to¡¡the¡¡second¡¡law¡¡of¡¡motion£»¡¡each¡¡one¡¡of¡¡the¡¡different¡¡forces£»¡¡operating¡¡at¡¡the¡¡same¡¡time¡¡upon¡¡a¡¡moving¡¡body£»¡¡produces¡¡the¡¡same¡¡effect¡¡as¡¡if¡¡it¡¡operated¡¡upon¡¡the¡¡body¡¡while¡¡at¡¡rest¡£
STEVINUS¡¡AND¡¡THE¡¡LAW¡¡OF¡¡EQUILIBRIUM¡¡It¡¡appears£»¡¡then£»¡¡that¡¡the¡¡mechanical¡¡studies¡¡of¡¡Galileo£»¡¡taken¡¡as¡¡a¡¡whole£»¡¡were¡¡nothing¡¡less¡¡than¡¡revolutionary¡£¡¡They¡¡constituted¡¡the¡¡first¡¡great¡¡advance¡¡upon¡¡the¡¡dynamic¡¡studies¡¡of¡¡Archimedes£»¡¡and¡¡then¡¡led¡¡to¡¡the¡¡secure¡¡foundation¡¡for¡¡one¡¡of¡¡the¡¡most¡¡important¡¡of¡¡modern¡¡sciences¡£¡¡We¡¡shall¡¡see¡¡that¡¡an¡¡important¡¡company¡¡of¡¡students¡¡entered¡¡the¡¡field¡¡immediately¡¡after¡¡the¡¡time¡¡of¡¡Galileo£»¡¡and¡¡carried¡¡forward¡¡the¡¡work¡¡he¡¡had¡¡so¡¡well¡¡begun¡£¡¡But¡¡before¡¡passing¡¡on¡¡to¡¡the¡¡consideration¡¡of¡¡their¡¡labors£»¡¡we¡¡must¡¡consider¡¡work¡¡in¡¡allied¡¡fields¡¡of¡¡two¡¡men¡¡who¡¡were¡¡contemporaries¡¡of¡¡Galileo¡¡and¡¡whose¡¡original¡¡labors¡¡were¡¡in¡¡some¡¡respects¡¡scarcely¡¡less¡¡important¡¡than¡¡his¡¡own¡£¡¡These¡¡men¡¡are¡¡the¡¡Dutchman¡¡Stevinus£»¡¡who¡¡must¡¡always¡¡be¡¡remembered¡¡as¡¡a¡¡co¡laborer¡¡with¡¡Galileo¡¡in¡¡the¡¡foundation¡¡of¡¡the¡¡science¡¡of¡¡dynamics£»¡¡and¡¡the¡¡Englishman¡¡Gilbert£»¡¡to¡¡whom¡¡is¡¡due¡¡the¡¡unqualified¡¡praise¡¡of¡¡first¡¡subjecting¡¡the¡¡phenomenon¡¡of¡¡magnetism¡¡to¡¡a¡¡strictly¡¡scientific¡¡investigation¡£¡¡Stevinus¡¡was¡¡born¡¡in¡¡the¡¡year¡¡1548£»¡¡and¡¡died¡¡in¡¡1620¡£¡¡He¡¡was¡¡a¡¡man¡¡of¡¡a¡¡practical¡¡genius£»¡¡and¡¡he¡¡attracted¡¡the¡¡attention¡¡of¡¡his¡¡non¡scientific¡¡contemporaries£»¡¡among¡¡other¡¡ways£»¡¡by¡¡the¡¡construction¡¡of¡¡a¡¡curious¡¡land¡craft£»¡¡which£»¡¡mounted¡¡on¡¡wheels£»¡¡was¡¡to¡¡be¡¡propelled¡¡by¡¡sails¡¡like¡¡a¡¡boat¡£¡¡Not¡¡only¡¡did¡¡he¡¡write¡¡a¡¡book¡¡on¡¡this¡¡curious¡¡horseless¡¡carriage£»¡¡but¡¡he¡¡put¡¡his¡¡idea¡¡into¡¡practical¡¡application£»¡¡producing¡¡a¡¡vehicle¡¡which¡¡actually¡¡traversed¡¡the¡¡distance¡¡between¡¡Scheveningen¡¡and¡¡Petton£»¡¡with¡¡no¡¡fewer¡¡than¡¡twenty¡seven¡¡passengers£»¡¡one¡¡of¡¡them¡¡being¡¡Prince¡¡Maurice¡¡of¡¡Orange¡£¡¡This¡¡demonstration¡¡was¡¡made¡¡about¡¡the¡¡year¡¡1600¡£¡¡It¡¡does¡¡not¡¡appear£»¡¡however£»¡¡that¡¡any¡¡important¡¡use¡¡was¡¡made¡¡of¡¡the¡¡strange¡¡vehicle£»¡¡but¡¡the¡¡man¡¡who¡¡invented¡¡it¡¡put¡¡his¡¡mechanical¡¡ingenuity¡¡to¡¡other¡¡use¡¡with¡¡better¡¡effect¡£¡¡It¡¡was¡¡he¡¡who¡¡solved¡¡the¡¡problem¡¡of¡¡oblique¡¡forces£»¡¡and¡¡who¡¡discovered¡¡the¡¡important¡¡hydrostatic¡¡principle¡¡that¡¡the¡¡pressure¡¡of¡¡fluids¡¡is¡¡proportionate¡¡to¡¡their¡¡depth£»¡¡without¡¡regard¡¡to¡¡the¡¡shape¡¡of¡¡the¡¡including¡¡vessel¡£¡¡The¡¡study¡¡of¡¡oblique¡¡forces¡¡was¡¡made¡¡by¡¡Stevinus¡¡with¡¡the¡¡aid¡¡of¡¡inclined¡¡planes¡£¡¡His¡¡most¡¡demonstrative¡¡experiment¡¡was¡¡a¡¡very¡¡simple¡¡one£»¡¡in¡¡which¡¡a¡¡chain¡¡of¡¡balls¡¡of¡¡equal¡¡weight¡¡was¡¡hung¡¡from¡¡a¡¡triangle£»¡¡the¡¡triangle¡¡being¡¡so¡¡constructed¡¡as¡¡to¡¡rest¡¡on¡¡a¡¡horizontal¡¡base£»¡¡the¡¡oblique¡¡sides¡¡bearing¡¡the¡¡relation¡¡to¡¡each¡¡other¡¡of¡¡two¡¡to¡¡one¡£¡¡Stevinus¡¡found¡¡that¡¡his¡¡chain¡¡of¡¡balls¡¡just¡¡balanced¡¡when¡¡four¡¡balls¡¡were¡¡on¡¡the¡¡longer¡¡side¡¡and¡¡two¡¡on¡¡the¡¡shorter¡¡and¡¡steeper¡¡side¡£¡¡The¡¡balancing¡¡of¡¡force¡¡thus¡¡brought¡¡about¡¡constituted¡¡a¡¡stable¡¡equilibrium£»¡¡Stevinus¡¡being¡¡the¡¡first¡¡to¡¡discriminate¡¡between¡¡such¡¡a¡¡condition¡¡and¡¡the¡¡unbalanced¡¡condition¡¡called¡¡unstable¡¡equilibrium¡£¡¡By¡¡this¡¡simple¡¡experiment¡¡was¡¡laid¡¡the¡¡foundation¡¡of¡¡the¡¡science¡¡of¡¡statics¡£¡¡Stevinus¡¡had¡¡a¡¡full¡¡grasp¡¡of¡¡the¡¡principle¡¡which¡¡his¡¡experiment¡¡involved£»¡¡and¡¡he¡¡applied¡¡it¡¡to¡¡the¡¡solution¡¡of¡¡oblique¡¡forces¡¡in¡¡all¡¡directions¡£¡¡Earlier¡¡investigations¡¡of¡¡Stevinus¡¡were¡¡published¡¡in¡¡1608¡£¡¡His¡¡collected¡¡works¡¡were¡¡published¡¡at¡¡Leyden¡¡in¡¡1634¡£¡¡This¡¡study¡¡of¡¡the¡¡equilibrium¡¡of¡¡pressure¡¡of¡¡bodies¡¡at¡¡rest¡¡led¡¡Stevinus£»¡¡not¡¡unnaturally£»¡¡to¡¡consider¡¡the¡¡allied¡¡subject¡¡of¡¡the¡¡pressure¡¡of¡¡liquids¡£¡¡He¡¡is¡¡to¡¡be¡¡credited¡¡with¡¡the¡¡explanation¡¡of¡¡the¡¡so¡called¡¡hydrostatic¡¡paradox¡£¡¡The¡¡familiar¡¡modern¡¡experiment¡¡which¡¡illustrates¡¡this¡¡paradox¡¡is¡¡made¡¡by¡¡inserting¡¡a¡¡long¡¡perpendicular¡¡tube¡¡of¡¡small¡¡caliber¡¡into¡¡the¡¡top¡¡of¡¡a¡¡tight¡¡barrel¡£¡¡On¡¡filling¡¡the¡¡barrel¡¡and¡¡tube¡¡with¡¡water£»¡¡it¡¡is¡¡possible¡¡to¡¡produce¡¡a¡¡pressure¡¡which¡¡will¡¡burst¡¡the¡¡barrel£»¡¡though¡¡it¡¡be¡¡a¡¡strong¡¡one£»¡¡and¡¡though¡¡the¡¡actual¡¡weight¡¡of¡¡water¡¡in¡¡the¡¡tube¡¡is¡¡comparatively¡¡insignificant¡£¡¡This¡¡illustrates¡¡the¡¡fact¡¡that¡¡the¡¡pressure¡¡at¡¡the¡¡bottom¡¡of¡¡a¡¡column¡¡of¡¡liquid¡¡is¡¡proportionate¡¡to¡¡the¡¡height¡¡of¡¡the¡¡column£»¡¡and¡¡not¡¡to¡¡its¡¡bulk£»¡¡this¡¡being¡¡the¡¡hydrostatic¡¡paradox¡¡in¡¡question¡£¡¡The¡¡explanation¡¡is¡¡that¡¡an¡¡enclosed¡¡fluid¡¡under¡¡pressure¡¡exerts¡¡an¡¡equal¡¡force¡¡upon¡¡all¡¡parts¡¡of¡¡the¡¡circumscribing¡¡wall£»¡¡the¡¡aggregate¡¡pressure¡¡may£»¡¡therefore£»¡¡be¡¡increased¡¡indefinitely¡¡by¡¡increasing¡¡the¡¡surface¡£¡¡It¡¡is¡¡this¡¡principle£»¡¡of¡¡course£»¡¡which¡¡is¡¡utilized¡¡in¡¡the¡¡familiar¡¡hydrostatic¡¡press¡£¡¡Theoretical¡¡explanations¡¡of¡¡the¡¡pressure¡¡of¡¡liquids¡¡were¡¡supplied¡¡a¡¡generation¡¡or¡¡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GALILEO¡¡AND¡¡THE¡¡EQUILIBRIUM¡¡OF¡¡FLUIDS¡¡Experiments¡¡of¡¡an¡¡allied¡¡character£»¡¡having¡¡to¡¡do¡¡with¡¡the¡¡equilibrium¡¡of¡¡fluids£»¡¡exercised¡¡the¡¡ingenuity¡¡of¡¡Galileo¡£¡¡Some¡¡of¡¡his¡¡most¡¡interesting¡¡experiments¡¡have¡¡to¡¡do¡¡with¡¡the¡¡subject¡¡of¡¡floating¡¡bodies¡£¡¡It¡¡will¡¡be¡¡recalled¡¡that¡¡Archimedes£»¡¡away¡¡back¡¡in¡¡the¡¡Alexandrian¡¡epoch£»¡¡had¡¡solved¡¡the¡¡most¡¡important¡¡problems¡¡of¡¡hydrostatic¡¡equilibrium¡£¡¡Now£»¡¡however£»¡¡his¡¡experiments¡¡were¡¡overlooked¡¡or¡¡forgotten£»¡¡and¡¡Galileo¡¡was¡¡obliged¡¡to¡¡make¡¡experiments¡¡anew£»¡¡and¡¡to¡¡combat¡¡fallacious¡¡views¡¡that¡¡ought¡¡long¡¡since¡¡to¡¡have¡¡been¡¡abandoned¡£¡¡Perhaps¡¡the¡¡most¡¡illuminative¡¡view¡¡of¡¡the¡¡spirit¡¡of¡¡the¡¡times¡¡can¡¡be¡¡gained¡¡by¡¡quoting¡¡at¡¡length¡¡a¡¡paper¡¡of¡¡Galileo's£»¡¡in¡¡which¡¡he¡¡details¡¡his¡¡own¡¡experiments¡¡with¡¡floating¡¡bodies¡¡and¡¡controverts¡¡the¡¡views¡¡of¡¡his¡¡opponents¡£¡¡The¡¡paper¡¡has¡¡further¡¡value¡¡as¡¡illustrating¡¡Galileo's¡¡methods¡¡both¡¡as¡¡experimenter¡¡and¡¡as¡¡speculative¡¡reasoner¡£¡¡The¡¡current¡¡view£»¡¡which¡¡Galileo¡¡here¡¡undertakes¡¡to¡¡refute£»¡¡asserts¡¡that¡¡water¡¡offers¡¡resistance¡¡to¡¡penetration£»¡¡and¡¡that¡¡this¡¡resistance¡¡is¡¡instrumental¡¡in¡¡determining¡¡whether¡¡a¡¡body¡¡placed¡¡in¡¡water¡¡will¡¡float¡¡or¡¡sink¡£¡¡Galileo¡¡contends¡¡that¡¡water¡¡is¡¡non¡resistant£»¡¡and¡¡that¡¡bodies¡¡float¡¡or¡¡sink¡¡in¡¡virtue¡¡of¡¡their¡¡respective¡¡weights¡£¡¡This£»¡¡of¡¡course£»¡¡is¡¡merely¡¡a¡¡restatement¡¡of¡¡the¡¡law¡¡of¡¡Archimedes¡£¡¡But¡¡it¡¡remains¡¡to¡¡explain¡¡the¡¡fact¡¡that¡¡bodies¡¡of¡¡a¡¡certain¡¡shape¡¡will¡¡float£»¡¡while¡¡bodies¡¡of¡¡the¡¡same¡¡material¡¡and¡¡weight£»¡¡but¡¡of¡¡a¡¡different¡¡shape£»¡¡will¡¡sink¡£¡¡We¡¡shall¡¡see¡¡what¡¡explanation¡¡Galileo¡¡finds¡¡of¡¡this¡¡anomaly¡¡as¡¡we¡¡proceed¡£¡¡In¡¡the¡¡first¡¡place£»¡¡Galileo¡¡makes¡¡a¡¡cone¡¡of¡¡wood¡¡or¡¡of¡¡wax£»¡¡and¡¡shows¡¡that¡¡when¡¡it¡¡floats¡¡with¡¡either¡¡its¡¡point¡¡or¡¡its¡¡base¡¡in¡¡the¡¡water£»¡¡it¡¡displaces¡¡exactly¡¡the¡¡same¡¡amount¡¡of¡¡fluid£»¡¡although¡¡the¡¡apex¡¡is¡¡by¡¡its¡¡shape¡¡better¡¡adapted¡¡to¡¡overcome¡¡the¡¡resistance¡¡of¡¡the¡¡water£»¡¡if¡¡that¡¡were¡¡the¡¡cause¡¡of¡¡buoyancy¡£¡¡Again£»¡¡the¡¡experiment¡¡may¡¡be¡¡varied¡¡by¡¡tempering¡¡the¡¡wax¡¡with¡¡filings¡¡of¡¡lead¡¡till¡¡it¡¡sinks¡¡in¡¡the¡¡water£»¡¡when¡¡it¡¡will¡¡be¡¡found¡¡that¡¡in¡¡any¡¡figure¡¡the¡¡same¡¡quantity¡¡of¡¡cork¡¡must¡¡be¡¡added¡¡to¡¡it¡¡to¡¡raise¡¡the¡¡surface¡£¡¡¡¨But£»¡¨¡¡says¡¡Galileo£»¡¡¡¨this¡¡silences¡¡not¡¡my¡¡antagonists£»¡¡they¡¡say¡¡that¡¡all¡¡the¡¡discourse¡¡hitherto¡¡made¡¡by¡¡me¡¡imports¡¡little¡¡to¡¡them£»¡¡and¡¡that¡¡it¡¡serves¡¡their¡¡turn£»¡¡that¡¡they¡¡have¡¡demonstrated¡¡in¡¡one¡¡instance£»¡¡and¡¡in¡¡such¡¡manner¡¡and¡¡figure¡¡as¡¡pleases¡¡them¡¡best¡¡namely£»¡¡in¡¡a¡¡board¡¡and¡¡in¡¡a¡¡ball¡¡of¡¡ebonythat¡¡one¡¡when¡¡put¡¡into¡¡the¡¡water¡¡sinks¡¡to¡¡the¡¡bottom£»¡¡and¡¡that¡¡the¡¡other¡¡stays¡¡to¡¡swim¡¡on¡¡the¡¡top£»¡¡and¡¡the¡¡matter¡¡being¡¡the¡¡same£»¡¡and¡¡the¡¡two¡¡bodies¡¡differing¡¡in¡¡nothing¡¡but¡¡in¡¡figure£»¡¡they¡¡affirm¡¡that¡¡with¡¡all¡¡perspicuity¡¡they¡¡have¡¡demonstrated¡¡and¡¡sensibly¡¡manifested¡¡what¡¡they¡¡undertook¡£¡¡Nevertheless£»¡¡I¡¡believe£»¡¡and¡¡think¡¡I¡¡can¡¡prove£»¡¡that¡¡this¡¡very¡¡experiment¡¡proves¡¡nothing¡¡against¡¡my¡¡theory¡£¡¡And¡¡first£»¡¡it¡¡is¡¡false¡¡that¡¡the¡¡ball¡¡sinks¡¡and¡¡the¡¡board¡¡not£»¡¡for¡¡the¡¡board¡¡will¡¡sink£»¡¡too£»¡¡if¡¡you¡¡do¡¡to¡¡both¡¡the¡¡figures¡¡as¡¡the¡¡words¡¡of¡¡our¡¡question¡¡require£»¡¡that¡¡is£»¡¡if¡¡you¡¡put¡¡them¡¡both¡¡in¡¡the¡¡water£»¡¡for¡¡to¡¡be¡¡in¡¡the¡¡water¡¡implies¡¡to¡¡be¡¡placed¡¡in¡¡the¡¡water£»¡¡and¡¡by¡¡Aristotle's¡¡own¡¡definition¡¡of¡¡place£»¡¡to¡¡be¡¡placed¡¡imports¡¡to¡¡be¡¡environed¡¡by¡¡the¡¡surface¡¡of¡¡the¡¡ambient¡¡body£»¡¡but¡¡when¡¡my¡¡antagonists¡¡show¡¡the¡¡floating¡¡board¡¡of¡¡ebony£»¡¡they¡¡put¡¡it¡¡not¡¡into¡¡the¡¡water£»¡¡but¡¡upon¡¡the¡¡water£»¡¡where£»¡¡being¡¡detained¡¡by¡¡a¡¡certain¡¡impediment¡¡£¨of¡¡which¡¡more¡¡anon£©£»¡¡it¡¡is¡¡surrounded£»¡¡partly¡¡with¡¡water£»¡¡partly¡¡with¡¡air£»¡¡which¡¡is¡¡contrary¡¡to¡¡our¡¡agreement£»¡¡for¡¡that¡¡was¡¡that¡¡bodies¡¡should