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Lecture7Thermodynamics:TheSecondandThirdLaws
HOT COLDq
DIRECTIONOFSPONTANEOUSCHANGES
Thedirectionofchangeisrelatedtothedistributionofenergy:spontaneouschangesarealwaysaccompaniedbyareductionofthe“quality”ofenergyfromamoreorganizedtoamoredispersed,chaoticform.
SPONTANEOUSCHANGE-CHAOTICDISPERSALOFTHETOTALENERGY
TOWARDSGREATERDISORDER
ANEWFUNCTIONOFSTATE:ENTROPY
ThedispersalofenergycanberelatedtotheheattransferredinaprocessTHERMODYNAMICDEFINITION:
ΔS=qrev/T(Clausius)
ThedispersalofenergycanbecalculatedSTATISTICALDEFINITION:S=kBlnW(Boltzmann)
SPONTANEOUS PROCESSES CAUSE AN INCREASE IN THE ENTROPYOFTHEUNIVERSEIRREVERSBLEPROCESSESARESPONTANEOUSIRREVERSIBLEPROCESSESGENERATEENTROPYREVERSIBLEPROCESSESDONOTGENERATEENTROPY(BUTTHEYMAYTRANSFERITFROMONEPARTOFTHEUNIVERSETOANOTHER)
THEQUANTITATIVEDEFINITIONOFENTROPY1)Thermodynamic(Clausius)
Sisastatefunctiondqrevisnotanexactdifferentialdqrev/Tisanexactdifferential
1/Tistheintegratingfactorofdqrev
ReversibleIsothermalExpansion
ForagasbehavingperfectlyPV=nRT
IrreversiblevsReversibleExpansion
PathA PathB
qirrev<qrev
CLAUSIUSINEQUALITY
Foranisolatedsystem:ΔS≥0
ΔSuniverse≥0
SecondLaw:TheentropyofanisolatedsystemincreasesInthecourseofaspontaneouschange.
ΔSuniverse= Δssystem+Δssurroundings≥0Δssystem≥-ΔSsurroundings
Example1
Overallentropychangeforanisothermalreversibleexpansion:
PathB
Overallentropychangeforanirreversiblefreeexpansion:
Example2
Heatflowfromahottoacoldbody
qTh Tc
THEENTROPYCHANGEWHENASYSTEMISHEATED
Inaphasetransition,heatistransferredreversiblybetweenthesystemanditssurroundings:
AbsoluteEntropy
Unlikeenthalpy-wehaveanabsolutescaleforentropy.ThirdLawofThermodynamic:IftheentropyofeveryelementinitsstablestateatT=0Kistakenaszero,everysubstancehasapositiveentropywhichatT=0becomeszero forallperfectcrystallinesubstances,includingcompounds.
Unlikeenthalpy -wehaveanabsolute scale for entropy.Third Law of Thermodynamic: If the entropy of everyelementinitsstablestateatT=0Kistakenaszero,everysubstancehasapositiveentropywhichatT=0becomeszero for all perfect crystalline substances, includingcompounds.
• Entropyisameasureofdisorder:– Inaphasechange:
• Solid Liquid Gas• Highlyordered Lessordered Verydisordered
Weseewhysolidsgliquidggasphase@roomtemp
• Sgas>>Sliquid>Ssolid
RelativeEntropy
THEGIBBSFREEENERGY
P,T=CONSTANT
Thisresultsuggeststhatwedefineanewstatefunction,theGibbsFreeEnergy:
G=H-TS
Thedirectionofspontaneouschangeisthedirectioninwhichthefreeenergydecreases.
ΔG:themaximumnon-p,VworkatT,p=const.
F=U-TS
THEHELMHOLTZFREEENERGY
V,T=CONSTANT
ΔF:themaximumworkatT,V=const.
THEQUANTITATIVEDEFINITIONOFENTROPY2)Statistical(Boltzmann)
Distributions,microstatesanddisorder
state
1
2
1
Wi=#configurations=#microstates
0.25
0.25
0.50
1
2
3
Pi =wi
wii=1
n
∑
1.00.80.60.40.20.0
WE
IGH
T2.01.51.00.50.0
(N–NT)
N = 2 1:2:1
Nstates=3=N+1Nmicrostates=4=22=2N
N=2
1.00.80.60.40.20.0
WE
IGH
T3.02.52.01.51.00.50.0
(N–NT)
N = 3 1:3:3:1
Nstates=4=N+1Nmicrostates=8=23=2N
N=3
1.00.80.60.40.20.0
WE
IGH
T
43210(N–NT)
N =4 1:4:6:4:1
Nmicrostates=16=24=2N
Nstates=5=N+1
N=4
1.00.80.60.40.20.0
WE
IGH
T543210
(N–NT)
N = 5 1:5:10:10:5:1
Nstates=6=N+1Nmicrostates=32=25=2N
1.00.80.60.40.20.0
WE
IGH
T
76543210(N–NT)
N = 7
Nmicrostates=128=27
1.00.80.60.40.20.0
WE
IGH
T
50403020100(N–NT)
N = 50
1.00.80.60.40.20.0
WE
IGH
T
6543210(N–NT)
N = 6
Nmicrostates=64=26
N=1.1258999068x1015
1
2
3
4
L RDistributions,microstatesanddisorder
1.00.80.60.40.20.0
WE
IGH
T
43210(N–NT)
N =4 1:4:6:4:1
1.00.80.60.40.20.0
WE
IGH
T
43210(N–NT)
N =4 1:4:6:4:1
1
2
3
4
1
23
4
3
1
2
4
1
2
3
4
Distributions,microstatesanddisorder
1
2
3
4
1 2
3 4
12
3 4
1
2
3
4
12
34
1
2
3
4
Wmax = max # microstates
Nature evolves toward Wmax
ΔU = ΔH = 0
1.00.80.60.40.20.0
WE
IGH
T
43210(N–NT)
N =4 1:4:6:4:1
Positionaldisorder:crystals
Weaddenergy
Weremoveenergy
Energeticdisorder
EK = 3
2RT
n1 + n2 +…+ nm =N
εK = 3
2kBT
ε1n1 + ε2n2 +…+ εmnm = EK
n1 + n2 +…+ nm =N = 100
ε1n1 + ε2n2 +…+ εmnm = EK = 10000
Egalitariandistribution
Feudaldistribution
Boltzmanndistribution
n1 + n2 +…+ nm =N ε1n1 + ε2n2 +…+ εmnm = EK
n2
n1
= e−
ε2−ε1( )kbT
�
nin j
= exp −ε i −ε j
kBT
⎛
⎝ ⎜ ⎜
⎞
⎠ ⎟ ⎟
nin j
= exp − ΔεkBT
⎛
⎝ ⎜
⎞
⎠ ⎟
1.0
0.8
0.6
0.4
0.2
0.0
Ene
rget
ic L
evel
s
14121086420Occupation Probability
T1 T2 T3
T3 > T2 > T1
Wmax = max # microstates
Nature evolves toward Wmax
Wmax=max#microstates
NatureevolvestowardWmax
W=W1✕ W2
S=kBlnW=kB(lnW1+lnW2)
S=ClnW=C(lnW1+lnW2)
• States,S.–Themicroscopicenergylevelsavailableinasystem.
• Microstates,W.– The particular way in which particles are distributed amongst the
states.Numberofmicrostates=W.• TheBoltzmannconstant,kB=1.38✕ 10-23J/K.
– Effectivelythegasconstantpermolecule=R/NA.
S=kB✕lnW
TheBoltzmannEquationforEntropy
ΔS=S2–S1=kB(lnW2–lnW1)=kBln2
ForoneparticleconsideranexpansionatT=cost
V2=2V1
W2=2W1
N =1ΔS=kBln2
ΔS=S2–S1=kB(lnW2–lnW1)=kBln22
FortwoparticlesconsiderthesameexpansionatT=costV2=2V1
W2/W1=2✕2(eachparticlemovesindependentlyoftheother)
N =2ΔS=kB✕2✕ln2
ForthreeparticlesconsiderthesameexpansionatT=costV2=2V1
W2/W1=2✕2✕2(eachparticlemovesindependentlyoftheother)
ΔS=S2–S1=kB(lnW2–lnW1)=kBln23
N =3ΔS=kB✕3✕ln2
ForNparticlesconsiderthesameexpansionatT=costV2=2V1
W2/W1=2N
ΔS=S2–S1=kB(lnW2–lnW1)=kBln2N
N =NΔS=kB✕N✕ln2
FromthethermodynamicdefinitionofΔS:
N =NΔS=kB✕N✕ln2=Rln2
LINKINGTHECHANGESINGIBBSFREEENERGYTOTHEEQUILIBRIUMCONSTANT
dU=δq+δw FirstLaw
Forareversiblechangeintheabsenceofnon-p,Vwork:δq=TdS(SecondLaw);δw=-pdVdU=TdS-PdVHowever,Uisastatefunction,dUisanexactdifferentialthisfundamentalequationholdsforanyreversibleorirreversiblechangeofaclosedsysteminvolvingnonon-p,Vwork.
FirstStep:CombiningtheFirstandSecondLaws
SecondStep:ManipulatingtheGibbsFunction
G=G(T,p)Thermodynamics
Mathematics
Compare
Similarly,onecanderive:GREAT
PHYSICISTS
HAVE
STUDIEDUNDER
VERY
FINETEACHERS
G=G(T,p)
ThirdStep:ThePressureDependenceoftheGibbsFunction
Foraperfectgas:
Byintegratingweobtain:
Letp’=p0=1bar�G=G0
ThemolarGibbsfunctionGm=G/nthusis:
Gm(p)iscalledtheCHEMICALPOTENTIALandisindicatedbythesymbolµ
Foraperfectgas andPVm=RTareequivalent
Proof:
FourthStep:AllowingForChangesInComposition
Ingeneral:G=G(p,T,n1,n2….)
CHEMICALPOTENTIAL
Forasinglecomponentµ=Gm=G/n
AtconstantT,p,ifweadddn1molesof1toamixture,GincreasesbydG=µ1dn1
Considerthesimplereaction:ADB
Foranamount-dnA=-dξofAthatisconsumed,anamountdnB=+dξforms.Atconstantp,T:
isthechangeintheGibbsfunctionpermoleofreactionatadefinedcompositionofthereactionmixture.
IfΔrG<0thereactionproceedsAgBIfΔrG>0thereactionproceedsAfBIfΔrG=0thereactionisatequilibrium
Fifthstep:linkingΔrGandtheequilibriumconstant
Atequilibrium:ΔrG=0andQ=Kp
A,Bperfectgases:
Theresultisvalidingeneral:aA+bBDcC+dD
Inthegasphase:
Insolution:
TemperaturedependenceofK
Gibbs-Helmholtzequation
Forachange(e.g.achangeofstate,achemicalreaction):
van’tHoffequation
LeChatelierprinciplemadequantitative!Exothermicreactions:increasedTfavoursthereactantsEndothermicreactions:increasedTfavourstheproducts
Integratingthevan’tHoffequation