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Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes and the “>” applies to irreversible processes. 3. The entropy of a pure substance in perfect crystalline form at absolute zero is 0 J/K.

Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

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Page 1: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Three Laws of Thermodynamics

1. ΔEuniv = 0 For the system: ΔE = q + w

2. ΔSuniv ≥ 0 For the system: ΔS ≥ q/T,

where the “=“ applies to reversible processes and the “>” applies to irreversible processes.

3. The entropy of a pure substance in perfect crystalline form at absolute zero is 0 J/K.

Page 2: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Gibbs Energy Change at Constant T,P

ΔG < 0

Process is spontaneous. ΔG is the maximum P-V work that can be obtained from the reaction at constant T or is all of the non-PV work that can be obtained at constant T and P.

ΔG = 0

Process is at equilibrium. (at constant T and P.)

ΔG > 0

Process is not spontaneous. A minimum energy ΔG (at constant T and P) must be supplied to the system for the reaction to take place (but the reverse reaction is spontaneous).

Page 3: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Gibbs EnergyThe change in Gibbs Energy ΔG is the maximum non-PV work that can be obtained from a chemical reaction at constant T and P (or the minimum energy that must be supplied to make the reaction happen).

There two ways to obtain ΔG°:

1. ΔrxnG° = ΣmΔfG°(products) – ΣnΔfG°( reactants)

(m and n represent the stoichiometric coefficients)

2. ΔG° = ΔH° – TΔS°

Page 4: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Conventions Used in Establishing Standard Gibbs Energy G°

State of Matter Standard State

Element ΔfG° is 0 if it is in its standard state at the specified T.

Solution 1 M

Gas 1 bar

Liquid pure liquid

Solid pure solid

Page 5: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Finding ΔG° at a T other than 25°C

ΔG°(T) = ΔH°(25°C) – TΔS°(25°C)

You may not use the ΔG° values in the Appendix. You must calculate ΔG° from ΔH°(25°C) and ΔS°(25°C).

(We make the assumption that ΔH°(25°C) and ΔS°(25°C) don’t change with T.)

Page 6: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Finding ΔG° at a T other than 25°C

How much energy must be added to 1 mole of water at 75°C to form 1 mole of water vapor at 1 bar and 75°C?

H2O(l, 75°C) H2O(g, 1 bar, 75°C)

ΔG°(75°C) = ΔH°(25°C) – TΔS°(25°C)ΔG°(75°C) = 44.01 kJ – 348 K (0.11892 kJ/K)

ΔG°(75°C) = 2.62 kJ

Page 7: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Finding ΔG° at a T other than 25°C

What is the maximum P-V work that can be obtained from 1 mole of water vapor condensing at 1 bar and 65°C ?

H2O(g, 1 bar, 65°C) H2O(l, 65°C)

ΔG°(65°C) = ΔH°(25°C) - TΔS°(25°C)ΔG°(65°C) = - 44.01 kJ - 338 K (- 0.11892 kJ/K)

ΔG°(65°C) = - 3.82 kJ

The physical change is spontaneous and produces 3.82 kJ of energy per mole of water vapor.

Page 8: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

How do ΔH° and ΔS° Affect ΔG°?

What causes the condensation of 1 mol of water vapor at 65°C and 1 bar pressure to be spontaneous?

H2O(g, 1bar, 65°C) H2O(l, 65°C)

ΔG°(65°C) = - 44.01 kJ - 338 K (- 0.11892 kJ/K) = - 44.01 + 40.194 = - 3.82 kJ

Answer: The exothermicity of the process is enough to overcome the decrease in entropy at 65°C.

Page 9: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

How do ΔH and ΔS Affect ΔG?

ΔG = ΔH - TΔS

ΔH ΔS ΔG - - - at low T, + at higher T - + - at all T (always spontaneous) + + + at low T, - at higher T + - + at all T (never spontaneous)

Page 10: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Finding ΔG Under Nonstandard Conditions

ΔG(T) = ΔG°(T) + RT ln Q

Q is the reaction quotient

R is the gas constant

R = 8.3145

Page 11: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

The Reaction Quotient Q

Q is found by putting values into the expression for the equilibrium

constant K.

N2(g) + 3H2(g) 2NH3(g)

The values here do NOT have to be equilibrium values.

The values here MUST BE equilibrium values.

3

2

)()(

)(

22

3

eqHeqN

eqNHP PP

PK

3

2

)()(

)(

22

3

HN

NH

PP

PQ

Page 12: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Finding ΔG Under Nonstandard Conditions

ΔG(T) = ΔG°(T) + RT ln QFind the change in Gibbs Energy for the formation of

ammonia at 298 K when the reaction mixture consists of 0.50 bar N2, 0.75 bar H2, and 2.00 bar NH3.

You must always write the equation for the reaction first.

ΔG is an extensive property, like ΔH and ΔS. Its value depends on the stoichiometry.

Page 13: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Finding ΔG Under Nonstandard Conditions

ΔG(T) = ΔG°(T) + RT ln QFind the Gibbs Energy for the formation of ammonia at 298 K when the reaction mixture consists of 0.50 bar N2,

0.75 bar H2, and 2.00 bar NH3.

N2(g) + 3H2(g) 2NH3 (g) 3

2

)()(

)(

22

3

HN

NH

PP

PQ

Page 14: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Finding ΔG Under Nonstandard Conditions

ΔG(T) = ΔG°(T) + RT ln QFind the Gibbs Energy for the formation of ammonia at 298 K when the reaction mixture consists of 0.50 bar N2, 0.75 bar H2, and 2.00 bar NH3.

N2(g, 1bar, 25°C) + 3H2(g, 1 bar, 25°C) 2NH3 (g, 1 bar, 25°C)

ΔG°(1 bar, 25°C) = - 33.32 kJ

ΔG = - 33.32 kJ + (8.3145 )(298K) (ln 18.963)

ΔG = - 33.32 kJ + 7291 J = - 33.32 kJ + 7.291 kJ = - 26.03 kJ

The fact that ΔG < 0 tells us that the reaction is spontaneous…and that the system is NOT at equilibrium.

Page 15: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Gibbs Energy and Equilibrium

ΔG(T) = ΔG°(T) + RT ln Q

At equilibrium, Q = K and ΔG = 0.

0 = ΔG°(T) + RT ln K(T)

ΔG°(T) = - RT ln K(T)

K(T) = e -ΔG°/RT

Page 16: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Calculating K from ΔG° Use Appendix C to calculate the equilibrium constant for the formation of 1 mole of ammonia at 25°C and at 450°C.

First, we write the equation for the reaction:

½N2(g) + H2(g) NH3(g)

For 450°C, we will need ΔH° and ΔS°. We will use these to calculate ΔG° for both temperatures.

ΔH° = - 46.19 kJ

ΔS° = -99.12 J/K = - 0.09912 kJ/K

ΔG°(25°C) = - 16.66 kJ (from Appendix C)

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Page 17: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Calculating K from ΔG° Use Appendix C to calculate the equilibrium constant for the formation of 1 mole of ammonia at 25°C.

½N2(g) + H2(g) NH3(g)

ΔG°(1 bar, 25°C) = - 16.66 kJ

23

Page 18: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Calculating K from ΔG° Use Appendix C to calculate the equilibrium constant for the formation of 1 mole of ammonia at 450°C.

½N2(g) + H2(g) NH3(g)

ΔG°(450°C) = - 46.19 - (723 K)(- 0.09912 kJ/K) = 25.47 kJ

23

The reaction is not spontaneous at 450°C under standard conditions. It takes 25.47 kJ of energy to make the reaction happen at this temperature.

23

2

21

2

3

)()(

)()450(

eqHeqN

eqNHP

PP

PCK

)723(3145.8

)47.25(

KKmol

JkJ

e

0145.0237.4 e

Page 19: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Calculating K from ΔG° The CRC Handbook of Chemistry and Physics gives ΔfG° = -623.42 kJ for carbonic acid and ΔfG° = -587.06 kJ for the bicarbonate ion, both at 25°C. Find Ka1 using this data.

First, we write the equation for the reaction:

H2CO3(aq) H+(aq) + HCO3-(aq)

ΔG°(1M, 25°C) = -587.06 - (-623.42) = 36.36 kJ

767.14)298(3145.8

)36360(

102.41

xeeeKK

Kmol

JJ

RT

G

a

Appendix D, Table 1 has Ka1 = 4.3 x 10-7

Page 20: Three Laws of Thermodynamics 1. ΔE univ = 0 For the system: ΔE = q + w 2. ΔS univ ≥ 0 For the system: ΔS ≥ q/T, where the “=“ applies to reversible processes

Calculating ΔG° from K Appendix D Table 3 gives the solubility product Ksp for copper(II) carbonate. Use this Ksp to find ΔG° for copper(II) carbonate dissolving in water at 25°C.

First, we write the equation for the reaction:

CuCO3(s) Cu2+(aq) + CO32-(aq)

ΔG° = - RT ln Ksp = - (8.3145 )(298 K) ln (2.3x10-10)

ΔG°(1M, 25°C) = 55.0 kJ

From the CRC Handbook of Chemistry and Physics:

ΔG° = 54.9 kJ...If this value is not zero, does it mean the system cannot be at equilibrium at 25°C?