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© Dario Bressanini Standard Gibbs Energy of Formation The standard Gibbs energy of formation is the standard reaction Gibbs energy of formation of a compound from its elements in their reference states. Just like enthalpy, the standard Gibbs energy of a reaction can be found using the standard Gibbs energy of formation for products and reactants. θ θ reactants θ m products θ m θ S T H G ν G ν G r r f f r What is r G 298 for the combustion of methane? CH 4 (g) +2O 2 (g) 2H 2 O (l) + CO 2 (g) 1 - 1 - 2 θ 4 θ 2 θ 2 θ θ mol kJ 817 mol kJ 0 2 7 . 50 237 2 394 ) ( O 2 ) ( CH ) ( O H 2 ) ( CO g G g G l G g G G f f f f r
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Page 1: © Dario Bressanini Spontaneita’ e Temperatura. © Dario Bressanini Reazioni Spontanee.

© Dario Bressanini

Standard Gibbs Energy of Formation

The standard Gibbs energy of formation is the standard reaction Gibbs energy of formation of a compound from its elements in their reference states.

Just like enthalpy, the standard Gibbs energy of a reaction can be found using the standard Gibbs energy of formation for products and reactants.

θθ

reactants

θ

mproducts

θ

m

θ

STH

GνGνG

rr

ffr

What is rG298 for the combustion of methane?

CH4 (g) +2O2 (g) 2H2O (l) + CO2 (g)

1-

1-

2

θ

4

θ

2

θ

2

θθ

mol kJ 817

mol kJ 027.502372394

)( O2)(CH

)( OH2)(CO

gGgG

lGgGG

ff

ffr

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© Dario Bressanini

The Gibbs Energy Change The Gibbs Energy Change (cont’d)(cont’d)

For the methane combustion reactionFor the methane combustion reaction11 CHCH44(g) + (g) + 22 O O22(g) (g) 1 1 COCO22(g) + (g) + 22 H H22O(l)O(l)

rrGG = = n npp ffGG (products) - (products) - n nrr ffGG (reactants) (reactants)

= = 2 2 ffGG [H [H22O(l)] + O(l)] + 11 ffGG [CO [CO22(g)] - ((g)] - (7/27/2 ffGG [O[O22(g)] + (g)] + 1 1 ffGG [CH [CH44(g)] )(g)] )

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Free Energy Change, Free Energy Change, G, G, and Spontaneityand Spontaneity

Example 15-16: Calculate Example 15-16: Calculate GGoo298298 for the reaction for the reaction

in Example 15-8. Use appendix K.in Example 15-8. Use appendix K.

C H + 5 O 3 CO + 4 H O

you do it

3 8 g 2 g 2 g 2 l

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

Example 15-17: Calculate Example 15-17: Calculate SSoo298298 for the following reaction. for the following reaction.

In example 15-8, we found that In example 15-8, we found that HHoo298298= = -2219.9 kJ-2219.9 kJ, and in , and in

Example 15-16 we found that Example 15-16 we found that GGoo298298= = -2108.5 kJ-2108.5 kJ..

C H + 5 O CO + 4 H O3 8 g 2 g 2 g 2 3 l

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

Example 15-17: Calculate Example 15-17: Calculate SSoo298298 for the following reaction. for the following reaction.

In example 15-8, we found that In example 15-8, we found that HHoo298298= = -2219.9 kJ-2219.9 kJ, and in , and in

Example 15-16 we found that Example 15-16 we found that GGoo298298= = -2108.5 kJ-2108.5 kJ..

C H + 5 O CO + 4 H O

G H T S

T S H G

3 8 g 2 g 2 g 2

o o o

o o o

3 l

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

C H + 5 O CO + 4 H O

G H T S

T S H G

SH G

T kJ

K or - 374

3 8 g 2 g 2 g 2

o o o

o o o

oo o

kJK

JK

3

2219 9 2108 5

2980 374

l

. ( . )

.

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

SSoo298 298 = = -374 J/K-374 J/K which indicates that the disorder of the which indicates that the disorder of the

system system decreasesdecreases .. For the reverse reaction,For the reverse reaction,

3 CO3 CO2(g)2(g) + 4 H + 4 H22OO(g) (g) CC33HH8(g)8(g) + 5 O + 5 O2(g)2(g)

SSoo298 298 = = +374 J/K+374 J/K which indicates that the disorder of which indicates that the disorder of

the system the system increasesincreases ..

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

Example 15-18: Use thermodynamic data to estimate Example 15-18: Use thermodynamic data to estimate the normal boiling point of water.the normal boiling point of water.

H O H O

equilibrium at BP G = 0

G = H - T S or H = T S

T =HS

2 2 gl

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

assume H@BP H

H H H

H

H kJ@25 C

298o

oH Oo

H Oo

o JK

o o

2 (g) 2 ( )

l

2418 2858

44 0

. ( . )

.

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

assume S@BP S

S S S

S

S or - 0.1188

298o

oH Oo

H Oo

o JK

o JK

kJK

2 (g) 2 ( )

l

188 7 69 91

118 8

. .

.

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The Temperature The Temperature Dependence of SpontaneityDependence of Spontaneity

T =HS

H

S

.0 kJ0.1188

K

370 K - 273 K = 97 C

o

o kJK

o

44

370

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Calculating Go from Enthalpy and Entropy Values–I

Problem: Potassium chlorate, one of the common oxidizing agents inexplosives, fireworks, and matchheads, undergoes a solid-state redoxreaction when heated, in which the oxidation number of Cl in the reactant is higher in one of the products and lower in the other (disproportionation):

Use Hof and So values to calculate Go

sys ( Gorxn) at 25oC for this

reaction.Plan: To solve for Go, use Ho

f values to calculate Horxn( Ho

sys),use So values to calculate So

rxn( Sosys), and apply Equation 20.6.

Solution: Calculating Hosys from Ho

f values (with Equation 6.8):

4 KClO3 (s) 3 KClO4 (s) + KCl(s)

Hosys = Ho

rxn = ∑m Hof(products) ∑n Ho

f(reactants)

= [3 mol KClO4 ( Hof of KClO4) + 1 mol KCl ( Ho

f of KCl)] - [4 mol KClO3 ( Ho

f of KClO3)]

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Calculating Go from Enthalpy and Entropy Values–II

Hosys = [3 mol (-432.8 kJ/mol) + 1 mol (-436.7 kJ/mol)]

- [4 mol (-397.7 kJ/mol)] = -144 kJ

Calculating Sosys from So values (with Equation 20.3):

Sosys = So

rxn = [3 mol KClO4 ( So of KClO4) + 1 mol KCl ( So of KCl)] - [4 mol KClO3 (So of KClO3)] = [3 mol (151.0 J/mol K) + 1 mol (82.6 J/mol K)] - [4 mol (143.1 J/mol K)] = - 36.8 J/K

. ..

Calculating Gosys at 298 K:

Gosys = Ho

sys - T Sosys = -144 kJ - [(298 K)(-36.8 J/K)(1kJ/1000 J)]

Gosys = -133 kJ

The reaction is spontaneous which isconsistent with Go < 0

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Effect of Temperature on Reaction SpontaneityThe temperature at which a reaction occurs influences the magnitude of the T S term. By scrutinizing the signs of H and S, we can predict the effect of temperature on the sign of G and thus on the spontaneity of a process at any temperature.

1. Reaction is spontaneous at all temperatures: Ho < 0, So > 0

2. Reaction is nonspontaneous at all temperatures: Ho > 0, So < 0

Temperature-independent cases (opposite signs)

2 H2O2 (l) 2 H2O(l) + O2 (g) Ho = -196 kJ and So = 125 J/K

3 O2 (g) 2 O3 (g) Ho = 286 kJ and So = - 137 J/KTemperature-dependent cases (same signs)

3. Reaction is spontaneous at higher temperature: Ho > 0 and So > 0

4. Reaction is spontaneous at lower temperature: Ho < 0 and So < 0

2 N2O(g) + O2 (g) 4 NO(g) Ho = 197.1 kJ and So = 198.2 J/K

2 Na(s) + Cl2 (g) 2 NaCl(s) Ho = - 822.2 kJ and So = - 181.7 J/K

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Determining the Effect of Temperature on Go–I

Problem: An important reaction in the production of sulfuric acid is theoxidation of SO2 (g) to SO3 (g):

At 298 K, Go = -141.6 kJ; Ho = -198.4 kJ; and So = -187.9 J/K.(a) Use the data to decide if this reaction is spontaneous at 25oC and how Go will change with increasing T.(b) Assuming Ho and So are constant with T, is the reaction spontaneous at 900.oC?

Plan: (a) We examine the sign of Go to see if the reaction is spontaneous and the signs of Ho and So to see the effect of T.(b) We use Equation 20.6 to calculate Go from the given Ho and So at the higher T (in K).

Solution: Continued on next slide.

2 SO2 (g) + O2 (g) 2 SO3 (g)

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Determining the Effect of Temperature on Go–II

Solution: (a) Since Go < 0, the reaction is spontaneous at 298 K: a mixture of SO2 (g), O2 (g), and SO3 (g) in their standard states (1 atm) willspontaneously yield more SO3 (g). With So < 0, the term -T So > 0 andbecomes more positive at higher T. Therefore, Go will be less negative, and the reaction less spontaneous, with increasing T.

(b) Calculating Go at 900.oC (T= 273 + 900. = 1173 K):

Go = Ho - T So = - 198.4 kJ - [(1173 K)(-187.9 J/K)(1 kJ/1000 J)] = 22.0 kJ

Since Go > 0, the reaction is nonspontaneous at higher T.

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Calculating G at Nonstandard Conditions–IProblem: The oxidation of SO2, which we discussed earlier, is too slow

at 298 K to be useful in the manufacture of sulfuric acid. To overcome this low rate, the process is conducted at an elevated temperature.(a) Calculate K at 298 K and at 973 K. Go

298 = -141.6 kJ/mol ofreaction as written; using Ho and So values at 973 K, Go

973 = -12.12 kJ/mol of reaction as written. (b) In experiments to determine the effect of temperature on reactionspontaneity, sealed containers are filled with 0.500 atm SO2, 0.0100 atm O2, and 0.100 atm SO3 and kept at 25oC and at 700oC. Inwhich direction, if any, will the reaction proceed to reach equilibrium at each temperature?(c) Calculate G for the system in part (b) at each temperature.Plan: (a) We know Go, T, and R, so we can calculate the K’s fromEquation 12.10.(b) Calculate Q, and compare it with each K from part (a).

2 SO2 (g) + O2 (g) 2 SO3 (g)

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Calculating G at Nonstandard Conditions–IIPlan : Continued(c) Since these are not standard-state pressures, we calculate G at eachT from Equation 20.11 with the values of Go (given) and Q [found inpart (b)].Solution: (a) Calculating K at the two temperatures:

At 298 K, the exponent isGo = -RT ln K so K = e-( G/RT)

- ( Go/RT) = - = 57.2-141.6 kJ/mol x 1000 J

1 kJ8.31 J/mol K x 298 K.

K = e-( G/RT) = e57.2 = 7 x 1024

So At 973 K, the exponent is

- ( Go/RT) = - = 1.50-12.12 kJ/mol x 1000 J

1 kJ8.31 J/mol K x 973 K.

K = e-( G/RT) = e1.50 = 4.5

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Calculating G at Nonstandard Conditions-III(b) Calculating the value of Q :

Since Q < K at both temperatures, the denominator will decrease and thenumerator increase–more SO3 will form–until Q equals K. However, at 298 K, the reaction will go far to the right before reaching equilibrium, whereas at 973 K, it will move only slightly to the right.

(c) Calculating G, the nonstandard free energy change, at 298 K and 973 K

Q = = = 4.00p2

SO3

p2SO2 x pO2

0.1002

0.5002 x 0.0100

G298 = Go + RT ln Q = -141.6 kJ/mol + (8.31 J/mol K x x 298 K x ln 4.00) = -138.2 kJ/mol

1 kJ1000 J

G973 = Go + RT ln Q = - 12.12 kJ/mol + (8.31 J/mol K x x 973 K x ln 4.00 = - 0.90 kJ/mol

1 kJ1000 J

.

.

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© Dario BressaniniFig. 20.12

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Is the dissolution of ammonium Is the dissolution of ammonium nitrate product-favored? nitrate product-favored?

If so, is it enthalpy- or entropy-driven?If so, is it enthalpy- or entropy-driven?

EXAMPLE 2:

NH4NO3(s) NH4NO3(aq)

Calculating Calculating GGoorxnrxn for for

NHNH44NONO33(s) (s)

9_amnit.mov20 m07vd1.mov

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GGoorxnrxn for for NHNH44NONO33(s) (s) NH NH44NONO33(aq)(aq)

From tables of thermodynamic data we find

Horxn = +25.7 kJ

Sorxn = +108.7 J/K or +0.1087 kJ/K

Gorxn = +25.7 kJ - (298 K)(+0.1087

kJ/K)

= -6.7 kJ

Reaction is product-favored

. . . in spite of positive Horxn.

Reaction is “entropy driven”

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Calculating Calculating GGoo

rxnrxn

EXAMPLE 3: Combustion of carbon

C(graphite) + O2(g) CO2(g)

Gorxn = Gf

o(CO2) - [Gfo(graph) +

Gfo(O2)]

Gorxn = -394.4 kJ - [ 0 + 0]

Note that free energy of formation of an element in its standard state is 0.

Gorxn = -394.4 kJ

Reaction is product-favored as expected.

GGoorxnrxn = = GGff

oo (products) - (products) - GGffoo (reactants) (reactants)

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GGoo for COUPLED CHEMICAL REACTIONS for COUPLED CHEMICAL REACTIONS

Reduction of iron oxide by CO is an example ofusing TWO reactions coupled to each other in orderto drive a thermodynamically forbidden reaction:

Fe2O3(s) 4 Fe(s) + 3/2 O2(g) Gorxn = +742 kJ

3/2 C(s) + 3/2 O2 (g) 3/2 CO2(g) Gorxn = -592 kJ

with a thermodynamically allowed reaction:

Overall : Fe2O3(s) + 3/2 C(s) 2 Fe(s) + 3/2 CO2(g)

Gorxn= +301 kJ @ 25oC

BUT Gorxn < 0 kJ for T > 563oC

See Kotz, pp933-935 for analysis of the thermite reaction

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Other examples of coupled Other examples of coupled reactions:reactions:

Copper smelting

Cu2S (s) 2 Cu (s) + S (s) Gorxn= +86.2 kJ

(FORBIDDEN) Couple this with:S (s) + O2 (g) SO2 (s) Go

rxn= -300.1 kJ

Overall: Cu2S (s) + O2 (g) 2 Cu (s) + SO2 (s)

Gorxn= +86.2 kJ + -300.1 kJ = -213.9 kJ (ALLOWED)

Coupled reactions VERY COMMON in Biochemistry :e.g. all bio-synthesis driven by

ATP ADP for which Horxn = -20 kJ

Sorxn = +34 J/K

Gorxn = -30 kJ @ 37oC

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2 NO2 NO22 N N22OO44

GGoorxnrxn = -4.8 kJ = -4.8 kJ

pure NOpure NO22 has has GGrxn rxn < 0.< 0. Reaction proceeds until Reaction proceeds until GGrxn rxn

= 0 - the minimum in = 0 - the minimum in G(reaction) - see graph.G(reaction) - see graph.

At this point, both NAt this point, both N22OO44 and and NONO22 are present, with more are present, with more NN22OO44..

This is a This is a product-favoredproduct-favored reaction. reaction.

Thermodynamics and KThermodynamics and Keqeq (2)(2)

9_G_NO2.mov20m09an1.mov

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NN22OO44 2 NO2 NO22

GGoorxnrxn = +4.8 kJ = +4.8 kJ

pure Npure N22OO44 has has GGrxnrxn < 0. < 0. Reaction proceeds until Reaction proceeds until

GGrxn rxn = 0 - the minimum in = 0 - the minimum in G(reaction) - see graph.G(reaction) - see graph.

At this point, both NAt this point, both N22OO44 and and NONO22 are present, with more are present, with more NONO22.. This is a This is a reactant-favored reactant-favored

reaction. reaction.

Thermodynamics and KThermodynamics and Keq eq (3)(3)

9_G_N2O4.mov20m09an2.mov

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Calculate K for the reactionCalculate K for the reaction

NN22OO44 2 NO 2 NO22 GGoorxnrxn = +4.8 kJ = +4.8 kJ

GGoorxnrxn = +4800 J = - (8.31 J/K)(298 K) ln K = +4800 J = - (8.31 J/K)(298 K) ln K

Gorxn = - RT lnK

lnK = -4800 J

(8.31 J/K)(298K) = - 1.94

Thermodynamics and KThermodynamics and Keqeq (5)(5)

When Gorxn > 0, then K < 1 - reactant favoured

When Gorxn < 0, then K >1 - product favoured

K = 0.14

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Consider the synthesis of methanol:

CO(g) + H2(g) CH3OH(l)

Calculate GG at at 25 25 ooCC for this reaction where CO(g) at 5.0 atm and H2(g) at 3.0 atm are converted to CH3OH(l) .

GGff(CH3OH(l))−166 −166

kJkJ

GGff(H2(g))00

GGff(CO(g))−137 kJ−137 kJ

Given:

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Cont’

GG = = GG + + RTRT ln( ln(QQ))GG GGff(CH3OH(l))GGff(CO(g))GGff(H2(g))

GG kJkJ

Q = 1

=1

(5) . (3)2PCO . P2H2

= 2.2 x 10-2

GG = = xx + (8.3145)( + (8.3145)(298298) ln( ) ln( 2.2 x 10-

2))= − 38 kJ / mol

We must use:

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The second law is the greatest good and the greatest bad on earth.

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The good: Life is possible.

We make machines that make other machines, machines that mow lawns, move mountains, and go to the moon.

We eat concentrated energy in the form of food, process that energy to synthesize complex biochemicals and run our organism, excreting diffused energy as body heat and less concentrated energy substances.

We use concentrated energy fuels to gather all kinds of materials from all parts of the world and, without any energetic limitation, arrange them in ways that please us.

We affect non-spontaneous reactions (pure metals from ores, synthesizing curative drugs from simple compounds, altering DNA).

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The bad: Life is always threatened.

All of the biochemical systems that run our bodies are maintained and regulated by feedback subsystems, composed of complex substances that are synthesized internally by thermodynamically nonspontaneous reactions, affected by utilizing energy ultimately transferred from the metabolism of food. When these feedback subsystems fail energy can no longer be processed to carry out the many reactions we need for life that are contrary to the direction predicted by the second law.

Every organic chemical of the 10,000 different kinds in our bodies is metastable, synthesized by a nonspontaneous reaction and kept from instant oxidation in air by activation energies.

Living creatures are energy processing systems that cannot function unless biochemical cycles operate synchronically to use energy to oppose second law predictions.

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GT,p S

time Changes in entropy of an isolated system with time. Entropy increases with time until equilibrium is reached

Change in the Gibbs free energy at constant temperature and pressure. Under these conditions G decreases during the course of a spontaneous change until equilibrium is reached.

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Gibbs Free EnergyGibbs Free Energy

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Chemical Potentials of the Ideal Chemical Potentials of the Ideal GasGas

Differentiating the chemical potential with Differentiating the chemical potential with temperaturetemperature

J,mP

J ST

PPlnRTSTS

J,mJ,m

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The Standard Chemical PotentialThe Standard Chemical Potential

For PFor P1 1 = P= P = 1 bar, we define the standard = 1 bar, we define the standard

state chemical potential state chemical potential

°°= = (T, 1bar)(T, 1bar)

bar 1

PlnRT)bar 1 ,T()T(

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The Chemical Potential for Real The Chemical Potential for Real GasesGases

The fugacity (f) represents the chemical The fugacity (f) represents the chemical potential of a real gas.potential of a real gas.

Define the fugacity coefficient Define the fugacity coefficient

= f / P= f / P For a real gasFor a real gas

PflnRT)bar 1 ,T()T(

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Obtaining Fugacity Coefficients Obtaining Fugacity Coefficients

Comparing the chemical potential of the Comparing the chemical potential of the real gas to the chemical potential of an real gas to the chemical potential of an ideal gas at the same pressure ideal gas at the same pressure

PPlnRT

PflnRTidreal

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Calculating Fugacity CoefficientsCalculating Fugacity Coefficients

The fugacity coefficients are obtained from The fugacity coefficients are obtained from the compression factors (Z) as shown the compression factors (Z) as shown below below

P

0

dPP

1ZlnRT

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Partial molar (molal) quantitiesPartial molar (molal) quantities

If system is If system is notnot simple, e.g. open system or simple, e.g. open system or mixtures, then for e.g. substances A and Bmixtures, then for e.g. substances A and B

(see lab manual, the five pages following error analysis)(see lab manual, the five pages following error analysis)

For constant For constant T,P T,P and and nnAA (e.g. 1 kg water in expt (e.g. 1 kg water in expt

2)2)

Find Find VV does not vary does not vary linearly with linearly with nnBB

dV T P n nV

TdT

V

PdP

V

ndn

V

ndn

P n n T n n T P n T P n

( , , , ), , , , , , , ,

A BA

AB

B

A B A B B A

dVV

ndn

T P n

BB

A, ,

Slope =

partial molar volume

V

nV V

T P nB

B m,B

A, ,

mB = moles solute / kg solvent

V

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Note: at constant Note: at constant TT and and PP, the total volume of the solution is:, the total volume of the solution is:

VVm,Am,A, , VVm,Bm,B are are constantconstant for a given composition for a given composition

i.e. think of making up a solution at constant composition. i.e. think of making up a solution at constant composition. ThenThen

V = VV = Vm,A m,A nnAA + + VVm,B m,B nnBB

A similar equation applies for A similar equation applies for anyany partial molar quantity. partial molar quantity.

dV V dn V dnn n

0 00 0

A A B B

A B

dV T P n nV

TdT

V

PdP

V

ndn

V

ndn

P n n T n n T P n T P n

( , , , ), , , , , , , ,

A BA

AB

B

A B A B B A

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BBBB ,,A,,A,,A,,AA

nPSnVSnPTnVTn

H

n

U

n

G

n

A

DEFINE the DEFINE the chemical potentialchemical potential, , or partial molar free energy, of Aor partial molar free energy, of A

The exact differential for The exact differential for GG is is

Compare with combined law eqn (CL.G)Compare with combined law eqn (CL.G) dG + SdT - VdP = dwdG + SdT - VdP = dwrev rev dwdw

dG = - SdT + VdP + dG = - SdT + VdP + iidndnii G=A+PVG=A+PV

dA+PdV+VdP = - SdT + VdP + dA+PdV+VdP = - SdT + VdP + iidndnii

dA = -PdV - SdT + dA = -PdV - SdT + iidndnii

andand

this the most useful defn., as it is the only one this the most useful defn., as it is the only one

written in terms of intensive variables.written in terms of intensive variables.

dG T P n nG

TdT

G

PdP

G

ndn

G

ndn

P n n T n n T P n T P n

( , , , ) ......., , , , , , , ,

A BA

AB

B

A B A B B A

AA

B

G

nT P n, ,

BABA ,,,,

,nnTnnP P

GV

T

GS

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© Dario Bressanini

Criteria for equilibrium:Criteria for equilibrium:

recall: recall: dG = - SdT + VdP + dG = - SdT + VdP + iidndnii

For a reversible, equilibrium process (we’ll take For a reversible, equilibrium process (we’ll take dwdwsuch as a phase change or chemical reaction (at const. such as a phase change or chemical reaction (at const. T, T, PP))

( ( iceice liquid liquid ))dn dn = 0 = 0

i.e. equilibrium requires i.e. equilibrium requires iceice liquid liquid

Hence Hence criteriacriteria for for equilibriumequilibrium equal equal T T thermal equilthermal equil equal equal PP mechanical equilmechanical equil equal equal chemical equilchemical equil

( ) ',dG dn dwT P i ii

ice liquid

dnice = dnliquid

i ii

dn 0


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