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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¡¡two¡¡later¡¡by¡¡numerous¡¡investigators£»¡¡including¡¡Newton£»¡¡but¡¡the¡¡practical¡¡refoundation¡¡of¡¡the¡¡science¡¡of¡¡hydrostatics¡¡in¡¡modern¡¡times¡¡dates¡¡from¡¡the¡¡experiments¡¡of¡¡Stevinus¡£

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