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时间:2019-03-08
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1、1TheFirstLawofThermodynamics1.1ELEMENTSOFTHERMODYNAMICSTERMINOLOGYThefirststepinthethermodynamicanalysisofanythingmustbethedefinitionoftheentitythatisbeingsubjectedtoanalysis.Werefertothisentity(col-lectionofmatter,regioninspace)asasystem.Althoughtheneedforexe-cutingthi
2、sfirstmoveandfordoingitonceandunambiguouslyisobvious,thetemptationisgreattoassumethesystemdefinitionitselfobviousandomitit.Thisisasourceofconfusion,ifnotoutrighterror.Paradoxicaldifferencesbetweentworesultsclaimedbytwoexpertswhoattack‘‘thesameproblem’’areoftenexplainedb
3、ytherealizationthatthetwoproblemsolversweremen-tallyaddressingdifferentsystems.Aswewillseeverysoon,theprecisedef-initionofthesystemiscriticalwhendeterminingthelocationandmagnitudeofthermodynamicirreversibility.Thetendencytoforgettodefinethesystemisduemainlytotradition.
4、Inconsiderablyolderdisciplinessuchassolid-bodymechanics,thesystemisindeedobvious,asthemeresketchingofabodyfocusestheattentionofbothproblemsolverandcritic.Influidmechanicsandheattransfer,thesystemisagainunderstoodoncetheboundaryconditionsnecessaryforsolvingtheNavier–Sto
5、kesequationsarespecified.However,eveninfluidmechanicsandheattransfer,theunambiguousdefinitionofthesystemisamustifthemethodisorderofmagnitudeorCOPYRIGHTEDMATERIALscaleanalysis[1]—thatis,iftheanalystreplacestheNavier–Stokesequationswithapproximatealgebraicstatementsthatcan
6、-notbesubjectedtoboundaryconditions.Todefinethesystemmeansalsotoidentifysharplythesystem’senviron-ment,orsurroundings.Theenvironmentistheportionofmatterorregioninspacethatresidesoutsidethesystemselectedforanalysis.Whatdifferentiatesbetweenthesystemanditsenvironmentisth
7、esurfacecalledboundary.Oneveryimportantdefiningfeaturethatsometimesfallspreytothesameforcesoftraditionisthattheboundaryisasurface,notanothersystem(notethatthethicknessofasurfaceiszero;therefore,theboundarycanneithercontain12THEFIRSTLAWOFTHERMODYNAMICSmatternorfillavolum
8、einspace).Saidanotherway,thevalueofapropertythatismeasuredatapointonthesurfacecalledboundarymustbesharedbyboththesystemandth
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