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7/28/2019 Chem131_Chapter5
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STANDARD THERMODYNAMIC FUNCTIONS
aA+ bB cC+ dD
Chemical reaction
A + bB = cC+ dD
Equilibrium
Need to define the zeros from which things are measured!(e.g., sea level, center of earth)
Standard sates of pure substances(denoted by superscript )
Solid and liquid: P = 1 bar and temperature = T
Gas: P = 1 bar, temperature = T, ideal gas
V
m,200
H
m,200
H
200molar quantity
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STANDARD THERMODYNAMIC FUNCTIONS
Standard enthalpy of a reaction
aA1 + bA2 cA3 + dA4
H
rxn,T H
T H
HT = cH
m,T(A3) + dH
m,T(A4) aH
m,T(A1) bHm,T(A2)
HT = 3H
m,T(A3) + 4H
m,T(A4) + 1H
m,T(A1) + 2Hm,T(A2)
H
T =i
iH
m,T(A
i)2
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STANDARD THERMODYNAMIC FUNCTIONS
Standard enthalpy of a reaction
H
T =
i
iH
m,T(Ai)
molar enthalpy of Ai in its standard state at temperature TH
m,T(Ai) =
U
m,T(Ai) = molar internal energy of Ai in its standard state at temperature T
Not measurable
Not interesting
Only changes matter!
H
T
tabulated, but not for every reaction...
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STANDARD THERMODYNAMIC FUNCTIONS
Standard enthalpy of formation
(tabulated, at least for some temperatures)
fH
T =
is the enthalpy change associated with the process offorming the substance of interest starting from theseparated components in the standard states of theirmost stable forms (temperature = T and pressure = 1 bar)
6 C(graphite, 298K, P) + 3 H2(ideal gas, 298K, P) C6H6(liquid, 298K, P
)
How can we calculate the enthalpy of formation of benzene at T = 298 K?
How can we calculate the enthalpy of formation of formaldehyde at T = 307 K?
C(graphite, 307K, P) + H2(ideal gas, 307K, P)
+
1
2 O2(ideal gas, 307K, P
)
H2CO(ideal gas, 307K, P
)
4
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STANDARD THERMODYNAMIC FUNCTIONS
6 C(graphite, 298K, P) + 3 H2(ideal gas, 298K, P) C6H6(liquid, 298K, P
)
How can we calculate the enthalpy of formation of benzene at T = 298 K?
How can we calculate the enthalpy of formation of formaldehyde at T = 307 K?
C(graphite, 307K, P) + H2(ideal gas, 307K, P)
+1
2O2(ideal gas, 307K, P
) H2CO(ideal gas, 307K, P)
fH
T = 0 for each element in its reference form
fH
T = 0 for graphite (at both 298 K and 307 K
fH
T = 0 for H2 (at both 298 K and 307 K
fH
T = 0 for O2 at 307 K
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STANDARD THERMODYNAMIC FUNCTIONS
Standard enthalpy of a reaction
aA1 + bA2 cA3 + dA4
H
T =
i
iH
m,T(Ai) =
i
ifH
T(Ai)
Reactants in standard states
at temperature T
Products in standard states
at temperature T
H
T
Elements in standard states
at temperature T
fH
T(reactants) fH
T(products)
H
T = fH
T(products)fH
T(reactants)6
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
fH
T =fH
T(step 1)
+fH
T(step 2)
+
fH
T(step 3)+fH
T(step 4)
+fH
T(step 5)
+fH
T(step 6)
6 steps & use the properties of a state function
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
Step 1: Enthalpy change associated with the hypothetical transformation from anideal gas at T and 1 bar to a real gas at T and 1 bar
Need to calculate Hreal from Hideal
H= Hideal Hreal = Ha +Hb +Hc
Real gas at T and P = 0 bar Ideal gas at T and P = 0 bar
Ha
Hb
Hc
Real gas at T and Po Ideal gas at T and PoH= Hideal Hreal
T = constant
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STANDARD THERMODYNAMIC FUNCTIONS
Real gas at T and Po Ideal gas at T and Po
Real gas at T and P = 0 bar Ideal gas at T and P = 0 bar
H= Hideal Hreal
H= Hideal Hreal = Ha +Hb +Hc
HaHb
Hc
T = constant
Hb = Ub + PVb Hb=
Ub
Ub = intermolecular interactions 0 P 0when
check the behavior ofreal gases according to
Boyles and Charleslaws
Hb = 010
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STANDARD THERMODYNAMIC FUNCTIONS
Real gas at T and Po Ideal gas at T and Po
Real gas at T and P = 0 bar Ideal gas at T and P = 0 bar
H= Hideal Hreal
H= Hideal Hreal = Ha +Hb +Hc
HaHb
Hc
T = constant
HP
T
= VTVHc
Hc =?
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STANDARD THERMODYNAMIC FUNCTIONS
Real gas at T and Po Ideal gas at T and Po
Real gas at T and P = 0 bar Ideal gas at T and P = 0 bar
H= Hideal Hreal
H= Hideal Hreal = Ha +Hb +Hc
HaHb
Hc
HP
T
= VTV
T = constant
Hc = 0
Hc
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
Step 1: Enthalpy change associated with the hypothetical transformation from anideal gas at T and 1 bar to a real gas at T and 1 bar
Real gas at T and Po Ideal gas at T and Po
Real gas at T and P = 0 bar Ideal gas at T and P = 0 bar
Need to calculate Hreal from Hideal
H= Hideal Hreal
Ha
Hb
Hc
T = constant
H= 0
P
(V TV)dP
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
Step 2: Enthalpy change associated with mixing the different substances at T and 1bar (more important for gases)
CHAPTER 6
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
Step 3: Enthalpy change associated with bringing the substances from T and Po toT and P of interest
H(step3) =
i
Hi(T, P T, P)
Hi = T
T
CP,idT+ P
P(Vi TVii)dP
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
Step 4: Enthalpy change associated with the reaction that leads to the formation ofthe compound of interest from the mixed elements at T and P.
Use of a calorimeter(see book for a description of how it works)
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
Step 5: Enthalpy change associated with bringing the substances from T and P atwhich they are formed to the standard conditions T and Po.
H(step5) =
i
Hi(T, P T, P)
Hi = T
TCP,idT+
P
P(Vi TVii)dP
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STANDARD THERMODYNAMIC FUNCTIONS
How to determine the enthalpy of formation
Step 6: Enthalpy change associated with the hypothetical transformation from areal gas at T and 1 bar to an ideal gas at T and 1 bar
Inverse process of step 1(now done for the newly formed gas species)
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STANDARD THERMODYNAMIC FUNCTIONS
Relation between Ho and Uo
H= U+ PV H= U+ PVconstant pressure
aA1 + bA2 cA3 + dA4
V
= cV
m,A3+ dV
m,A4 aV
m,A1 bV
m,A2
H= U
+ P
V
volume change of solids and
liquids is small
V
i,gases
iV
m,i
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STANDARD THERMODYNAMIC FUNCTIONS
Relation between Ho and Uo
H= U+ PV H= U+ PVconstant pressure
H= U
+ P
V
aA1 + bA2 cA3 + dA4
V
= cV
m,A3+ dV
m,A4 aV
m,A1 bV
m,A2
V
i,gases
iV
m,i
V
m,i=
RT
P
V
m,i = ngRT
P
i,gases
i = ng
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STANDARD THERMODYNAMIC FUNCTIONS
Relation between Ho and Uo
H= U+ PV H= U+ PVconstant pressure
H = U
+ PV
aA1 + bA2 cA3 + dA4
H
= U
+ngRT
H
U
if there are no gases
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STANDARD THERMODYNAMIC FUNCTIONS
Hesss law
Often the reaction that forms a compound from its elements cannot be done.
Ho cannot be determined directly2C(graphite) + 3H2(g) C2H6(g)
2H6(g) +7
2O2(g) 2CO2(g) + 3H2O(l)
(graphite) + O2(g) CO2(g)
H2(g) +1
2O2(g) H2O(l)
H
1
H
2
H
3
(1)
(2)
(3)
2C(graphite) + 3H2(g) C2H6(g) (1) + 2 (2) + 3 (3)
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STANDARD THERMODYNAMIC FUNCTIONS
Hesss law
Often the reaction that forms a compound from its elements cannot be done.
Ho cannot be determined directly2C(graphite) + 3H2(g) C2H6(g)
2H6(g) +7
2O2(g) 2CO2(g) + 3H2O(l)
(graphite) + O2(g) CO2(g)
H2(g) +1
2O2(g) H2O(l)
H
1
H
2
H
3
(1)
(2)
(3)
H
= H
1+ 2H
2+ 3H
3
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STANDARD THERMODYNAMIC FUNCTIONS
Temperature dependence ofHo
We know Ho at T1 and we would like to know Ho at T2: dH
dT=?
dH
dT=
i
i
dH
m,i
dT
dH
dT=
i
iC
P,m,i = C
P
H
T2H
T1=
T2
T1
C
PdT
Kirchhoffs Law
24
S O C C O S
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STANDARD THERMODYNAMIC FUNCTIONS
Temperature dependence ofHo
H
T2H
T1=
T2
T1
C
PdT
Kirchhoffs Law
H
T2H
T1 C
P(T2 T1)
C
P,m = a+ bT+ cT2+ dT
3
IfT is small:
Otherwise use Kirchhoffs law with:
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
Conventional entropies
A lot of bookkeeping... in the end we are interested inS
(1) Choose an arbitrary value (=0) for entropy of each element in a chosenreference state (T=0, Po)
(2) Tabulate Sfor any change from elements in the chosen reference state tothe desired substance in a standard state
Entropy reference state
Pure element in its stable condensed form (solid or liquid) at 1 bar in the limit T 0 K
Arbitrary definition
S
m,0 = limT0
S
m,T = 0
pure element in its stable condensed form
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
How about So at T > 0 K?
If there is a phase change...
S= S
T S
0=
T
0
Cp
TdT
S=
Tpc0
Cp
TdT+Spc +
TTpc
Cp
TdT
How about the conventional entropy of a compound?
Its complicated!
S=qrev
T
a chemical reaction is an irreversible process!
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
Third law of thermodynamics
Measurements ofG for several reactions led Nernst (1907) to postulate
limT0
G
T
P
= 0
G
T
P
= S
G
T
P
= S
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
Third law of thermodynamics
Measurements ofG for several reactions led Nernst (1907) to postulate
limT0
G
T
P
= 0
G
T
P
= S
G
T
P
= S
limT0
S = 0
Important
not true when the substances involved in the reaction are not in internal equilibriume.g., supercritical liquids
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
Third law of thermodynamics
For any isothermal process that involves only substances in internal equilibrium,the entropy change goes to zero as T goes to zero
limT0
S = 0
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
How to calculate conventional entropies
A+B C
S
= 0 S
= 0 S
= 0
element element compound
T 0
T = 0 S=?
S= Sm,T2 =Tfus0
Cp,m(solid)T
dT+
fusH
m
T+
T2Tfus
Cp,m(liquid)T
dT+ . . .
there may be otherphase changes
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
How to calculate conventional entropies
S= Sm,T2 =
Tfus0
Cp,m(solid)
TdT+
fusH
m
T+
T2Tfus
Cp,m(liquid)
TdT+ . . .
If gases are involved we need to calculate the entropy change associated to thehypothetical transformation from an ideal gas at P = 1 bar and T to a real gas at P =
1 bar and T
S(ideal,T,P) S(real,T,P)
Real gas at T and P = 0 bar Ideal gas at T and P = 0 bar
Real gas at T and Po Ideal gas at T and Po
T = constantSa
Sb
Sc
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
How to calculate conventional entropies
S(ideal,T,P
)
S(real,T,P
)
Real gas at T and P = 0 bar Ideal gas at T and P = 0 bar
Real gas at T and Po Ideal gas at T and Po
T = constantSa
Sb
Sc
SP
T
=
VT
P
For steps a and c
Sb = 0In the limit T0, the entropy of ideal and real gasesbecome equal (statistical mechanics, Chem 132)
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
Standard enthalpy of reaction
S
T =
i
iS
m,T,i
usually tabulated at T = 298 K
ST2= S
T1+
T2
T1
CP
TdT+phase change contributions
At different T,
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STANDARD THERMODYNAMIC FUNCTIONS
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STANDARD THERMODYNAMIC FUNCTIONS
Standard Gibbs energy of reaction
aA+ bB cC+ dD
pure separated products intheir standard states at T
pure separated reactants intheir standard states at T
G
T =
i
iG
m,T,i G
T =
i
ifG
T,i
fG
T = fH
T,i TfS
T,i
enthalpies of formation from So and 3rd law of thermodynamics