Consider a wellinsulated pistoncylinder assembly On the 005 m piston rests two 5000kg blocks The initial temperature is 500 K The ambient pressure is 5 bar One mole of an ideal gas is contained in the cylinder The gas is compressed in a process in w ID: 50272
Download Pdf The PPT/PDF document "CYL I semester Homework Solutions" is the property of its rightful owner. Permission is granted to download and print the materials on this web site for personal, non-commercial use only, and to display it on your personal computer provided you do not modify the materials and that you retain all copyright notices contained in the materials. By downloading content from our website, you accept the terms of this agreement.
3.Asalespersonclaimsthatamysteriousblackbox,withnomovingparts,cantakeaninletstreamofidealgasat2kg/sand4barand50andcool0.5kg/sofitto10and1barwhiletherestofthegasisraisedto70at1bar.Isthispossible?Explain.(i)Massisconserved(ii)Energyisconserved:0:5kg=sCP(1050)K=1:5kg=sCP(7050)K(iii)Doesthesecondlawhold?Foranadiabaticprocess,dS dtuniv=0:5kg=s(S2S1)+1:5kg=s(S3S1)S2S1=CplnT2=T1RlnP2=P1S3S1=CplnT3=T1RlnP3=P1dS dtuniv=0:5kg=sCP(ln263+3ln3434ln323)+2Rln4SecondlawholdsaslongasCP218R,whichistrueforallimaginablegases.4.Calculatethemaximumworkandthemaximumnon-expansionworkthatcanbeobtainedfromthefreezingofsupercooledwaterat5and1.0atm.Thedensitiesofwaterandiceare0.999and0.917gcm3,respectivelyat5.ThesimplestprocedureistocalculatethechangeinGandAbyusingtherelationshipA=UTSamdG=HTS.FromthermodynamictablesweknowthatH=6008J/molforfreezingat0,CPforliquidwateris75J/(molK),andCPforiceis36.4J/(molK).ThecomputationofHandSwasdiscussedinclass.Asazerothapproximation,wecouldtakethatU=Hbecausecondensedphasesareinvolved.WecoulddobetterbyusingthedensitiestondthePdVcontributiontoH.H(268K)=H(273K)+(CP(solid)CP(liquid))(5K)U(268K)=H(268K)1atm(Vm(solid)Vm(liquid))S(268K)5.OnemoleofHeisheatedfrom200to400ataconstantpressureof1atm.GiventhattheabsoluteentropyofHeat200is810JK1mol1,andassumingHeisaperfectgas,commentonthespontaneityoftheprocess.S=S0+CPln673=473Thespontaneityoftheprocesswillbedeterminedbyhowtheheatingisdone.Iftheheatingisachievedbyputtingthegasintoaheatbathat400,thenStot=Ssys+Ssurr0:Ssurr=Hsys=673;Hsys=CP(200K)6.Derivetherelations:(i)CpCv=T@P @TV@V @TP;@H @TP@U @TVUsethedenitionH=U+PV@H @TP@U @TV=@U @TP+P@V @TP@U @TVToobtainanexpressionfor@U @TPweproceedasfollowsdU=@U @TVdT+@U @VTdVDividingbydTandapplyingconstantpressuregives@U @TP=@U @TV+@U @VT@V @TP:ThuswehaveCPCV=@U @VT@V @TP+P@V @TPUsingtheresultthatwasprovedinclass@U @VT=T@P @TVP 9.Thevaporpressureofzincvarieswithtemperatureaslogp(mmHg)=6850 T0:755logT+11:24andthatofliquidzincaslogp(mmHg)=6620 T1:255logT+12:34:Calculate(a)theboilingpointofzincAttheboilingpoint,thevaporpressureoftheliquidbecomestheatmosphericpressure,whichis760mmofHg.log760=6620 T1:255logT+12:34Wesolvethisbythemethodofsuccessiveapproximation.IdropthelogTtermtobeginwithandsolveforT.ThisgivesmeaninitialguessfortheroottobeT=699:85.IusethisguessrootinthelogTandsolvetheequationlog760=6620 T1:255log699:85+12:34forT,whichyieldsT=1124:1.IrepeatthisprocessafewtimesandndthatT=1181.Thereareothermethodstosolvethis-graphicalandusingacomputeralgebrasystemaretwopossibilities.(b)thetriplepointAtthetriplepoint,thesolid-vaporandliquid-vaporcoexistencecurvesintersect.Thismeans6620 T1:255logT+12:34=6850 T0:755logT+11:24230 T0:5logT+1:10=0Solvingthisequationwendthatthetemperatureatthetriplepointiscloseto700.OneusesthisTinoneoftheequationstondtheP.(c)theheatofevaporationattheboilingpoint2:303logp(mmHg)=lnP=2:3036620 T1:255logT+12:34:dlnP=2:303RdT6620 RT21:255 RT=2:303R66201:255T RT2dTComparingthiswiththeClausius-Clapeyronequation,dlnP=H=RT2dT,showsthatH=2:303R(66201:255T).SubstitutetheboilingpointT=1181inH=2:303R(66201:255T)andobtainH.(d)theheatoffusionTheheatoffusion,whichistheenthalpyofmelting,maybeobtainedfromsubtractingtheheatofevaporationfromtheheatofsublimation.Theheatofsublimationisobtainedbyfollowingthesameprocedureasinpart(c)forthesublimationcurve.(e)thedierenceintheCpsofsolidandliquidzinc.IfHhastheformA+BT,thenitimpliesthatB=CP.FromthetemperaturedependentpartofHforevaporationandsublimation,wecanobtainthedierenceintheCP's.10.ThePlanckfunctiondenedasY=H T+SisathermodynamicpotentialsimilartotheGibbsenergy.Obtaina\TdS"typeequationfordYandfromitaMaxwellrelation.Also,whatisthethermodynamiccriterionforspontaneityintermsofY.dY=H T2dTdH T+dS=H T2dT1 T(dHTdS)WeknowthatdH=TdSVdPsothatdY=H T2dTV TdPComparingthiswithdY=@Y @TPdT+@Y @PTdP