The Analyst

第2章

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第2章

The Analyst Katzenbach, John

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The Analyst
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  27。As,ontheonehand,itwereabsurdtogetridofobysaying,Letmecontradictmyself;letmesubvertmyownhypothesis;letmetakeitforgrantedthatthereisnoincrement,atthesametimethatIretainaquantitywhichIcouldneverhavegotatbutbyassuminganincrement:so,ontheotherhand,itwouldbeequallywrongtoimaginethatinageometricaldemonstrationwemaybeallowedtoadmitanyerror,thougheversosmall,orthatitispossible,inthenatureofthings,anaccurateconclusionshouldbederivedfrominaccurateprinciples。Thereforeocannotbethrownoutasaninfinitesimal,orupontheprinciplethatinfinitesimalsmaybesafelyneglected;butonlybecauseitisdestroyedbyanequalquantitywithanegativesign,whenceo-poisequaltonothing。Andasitisillegitimatetoreduceanequation,bysubductingfromonesideaquantitywhenitisnottobedestroyed,orwhenanequalquantityisnotsubductedfromtheothersideoftheequation:soitmustbeallowedaverylogicalandjustmethodofarguingtoconcludethatiffromequalseithernothingorequalquantitiesaresubductedtheyshallstillremainequal。Andthisisatruereasonwhynoerrorisatlastproducedbytherejectingofo。Whichthereforemustnotbeascribedtothedoctrineofdifferences,orinfinitesimals,orevanescentquantities,ormomentums,orfluxions。

  28。Supposethecasetobegeneral,andthatisequaltotheareaABCwhencebythemethodoffluxionstheordinateisfound,whichweadmitfortrue,andshallinquirehowitisarrivedat。Nowifwearecontenttocomeattheconclusioninasummaryway,bysupposingthattheratioofthefluxionsofxandisfound[Sect。13。]tobe1and,andthattheordinateoftheareaisconsideredasitsfluxion,weshallnotsoclearlyseeourway,orperceivehowthetruthcomesout,thatmethodaswehaveshewedbeforebeingobscureandillogical。Butifwefairlydelineatetheareaanditsincrement,anddividethelatterintotwopartsBCFDandCFH,[Seethefigureinsect。26。]andproceedregularlybyequationsbetweenthealgebraicalandgeometricalquantities,thereasonofthethingwillplainlyappear。ForasisequaltotheareaABC,soistheincrementofequaltotheincrementofthearea,i。e。toBDHC;thatistosayAndonlythefirstmembersoneachsideoftheequationbeingretained,=BDFC:anddividingbothsidesbyoorBD,weshallget=BC。AdmittingthereforethatthecurvilinearspaceCFHisequaltotherejectaneousquantityandthatwhenthisisrejectedononeside,thatisrejectedontheother,thereasoningbecomesjustandtheconclusiontrue。AnditisallonewhatevermagnitudeyouallowtoBD,whetherthatofaninfinitesimaldifferenceorafiniteincrementeversogreat。Itisthereforeplainthatthesupposingtherejectaneousalgebraicalquantitytobeaninfinitelysmallorevanescentquantity,andthereforetobeneglected,musthaveproducedanerror,haditnotbeenforthecurvilinearspacesbeingequalthereto,andatthesametimesubductedfromtheotherpartorsideoftheequation,agreeablytotheaxiom,Iffromequalsyousubductequals,theremainderswillbeequal。Forthosequantitieswhichbytheanalystsaresaidtobeneglected,ormadetovanish,areinrealitysubducted。Ifthereforetheconclusionbetrue,itisabsolutelynecessarythatthefinitespaceCFHbeequaltotheremainderoftheincrementexpressedbyequal,Isay,tothefiniteremainderofafiniteincrement。

  29。Therefore,bethepowerwhatyouplease,therewillariseononesideanalgebraicalexpression,ontheotherageometricalquantity,eachofwhichnaturallydividesitselfintothreemembers。Thealgebraicalorfluxionaryexpression,intoonewhichincludesneithertheexpressionoftheincrementoftheabscissanorofanypowerthereof;anotherwhichincludestheexpressionoftheincrementitself;andthethirdincludingtheexpressionofthepowersoftheincrement。Thegeometricalquantityalsoorwholeincreasedareaconsistsofthreepartsormembers,thefirstofwhichisthegivenarea;thesecondarectangleundertheordinateandtheincrementoftheabscissa;thethirdacurvilinearspace。And,comparingthehomologousorcorrespondentmembersonbothsides,wefindthatasthefirstmemberoftheexpressionistheexpressionofthegivenarea,sothesecondmemberoftheexpressionwillexpresstherectangleorsecondmemberofthegeometricalquantity,andthethird,containingthepowersoftheincrement,willexpressthecurvilinearspace,orthirdmemberofthegeometricalquantity。Thishintmayperhapsbefurtherextended,andappliedtogoodpurpose,bythosewhohaveleisureandcuriosityforsuchmatters。TheuseImakeofitistoshew,thattheanalysiscannotobtaininaugmentsordifferences,butitmustalsoobtaininfinitequantities,betheyeversogreat,aswasbeforeobserved。

  30。Itseemstherefore,uponthewhole,thatwemaysafelypronouncetheconclusioncannotberight,ifinordertheretoanyquantitybemadetovanish,orbeneglected,exceptthateitheroneerrorisredressedbyanother;orthat,secondly,onthesamesideofanequationequalquantitiesaredestroyedbycontrarysigns,sothatthequantitywemeantorejectisfirstannihilated;or,lastly,thatfromoppositesidesequalquantitiesaresubducted。Andthereforetogetridofquantitiesbythereceivedprinciplesoffluxionsorofdifferencesisneithergoodgeometrynorgoodlogic。Whentheaugmentsvanish,thevelocitiesalsovanish。Thevelocitiesorfluxionsaresaidtobeprimoandultimo,astheaugmentsnascentandevanescent。Takethereforetheratiooftheevanescentquantities,itisthesamewiththatofthefluxions。Itwillthereforeanswerallintentsaswell。Whythenarefluxionsintroduced?Isitnottoshunorrathertopalliatetheuseofquantitiesinfinitelysmall?Butwehavenonotionwherebytoconceiveandmeasurevariousdegreesofvelocitybesidesspaceandtime;or,whenthetimesaregiven,besidesspacealone。Wehaveevennonotionofvelocityprescindedfromtimeandspace。Whenthereforeapointissupposedtomoveingiventimes,wehavenonotionofgreaterorlesservelocities,orofproportionsbetweenvelocities,butonlyoflongerandshorterlines,andofproportionsbetweensuchlinesgeneratedinequalpartsoftime。

  31。Apointmaybethelimitofaline:alinemaybethelimitofasurface:amomentmayterminatetime。Buthowcanweconceiveavelocitybythehelpofsuchlimits?Itnecessarilyimpliesbothtimeandspace,andcannotbeconceivedwithoutthem。Andifthevelocitiesofnascentandevanescentquantities,i。e。abstractedfromtimeandspace,maynotbecomprehended,howcanwecomprehendanddemonstratetheirproportions;orconsidertheirrationesprimaeandultimae?

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