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Unit 5 - Chpt 17 - Thermochemistry Part II • Thermo - Entropy and Free Energy HW set1: Chpt 17 - pg. 807-815 #24, 25, 27-30, 32, 34, 36 Due Tues. Jan 29 HW set2: Chpt 17 pg. 807-815 # 40 - 42, 50, 54 Due Fri Feb 1 HW set3: Chpt 17 pg. 807-815 # 60, 64, 66, 71, 72, 109 Due Tues Feb 5

Unit 5 - Chpt 17 - Thermochemistry Part II

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Unit 5 - Chpt 17 - Thermochemistry Part II. Thermo - Entropy and Free Energy HW set1: Chpt 17 - pg. 807-815 #24, 25, 27-30, 32, 34, 36 Due Tues. Jan 29 HW set2: Chpt 17 pg. 807-815 # 40 - 42, 50, 54 Due Fri Feb 1 - PowerPoint PPT Presentation

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Page 1: Unit 5 - Chpt 17 - Thermochemistry Part II

Unit 5 - Chpt 17 - Thermochemistry Part II

• Thermo - Entropy and Free Energy• HW set1: Chpt 17 - pg. 807-815 #24, 25, 27-30,

32, 34, 36 Due Tues. Jan 29• HW set2: Chpt 17 pg. 807-815 # 40 - 42, 50, 54

Due Fri Feb 1 • HW set3: Chpt 17 pg. 807-815 # 60, 64, 66, 71,

72, 109 Due Tues Feb 5

Page 2: Unit 5 - Chpt 17 - Thermochemistry Part II

Spontaneous Process

• Reminder... 1st law of thermodynamics - the energy of the universe is a constant.

• Spontaneous reactions occur without outside intervention. Can be fast of slow. Thermodynamics can tell us direction of reaction, but say nothing about speed.

• Driving forces of reactions... 1. energy (exothermic) and 2. increase in entropy (chaos)... ice melting is endothermic

Page 3: Unit 5 - Chpt 17 - Thermochemistry Part II

Entropy (chaos, disorder)

Statistically which distribution is more likely?

Page 4: Unit 5 - Chpt 17 - Thermochemistry Part II

Entropy of phases of matter

Page 5: Unit 5 - Chpt 17 - Thermochemistry Part II

Concept check

Predict the sign of ΔS for each of the following, and explain:a)The evaporation of alcohol

b)The freezing of water

c)Compressing an ideal gas at constant temperature

d)Heating an ideal gas at constant pressure

e)Dissolving NaCl in water

+

+

+

Page 6: Unit 5 - Chpt 17 - Thermochemistry Part II

2nd Law of Themodynamics

• In any spontaneous reaction there is always an increase in the entropy of the universe. THE ENTROPY OF THE UNIVERSE IS INCREASING.

• System vs. Surroundings?

ΔSuniverse = ΔSsystem + ΔSsurroundings

Page 7: Unit 5 - Chpt 17 - Thermochemistry Part II

Ice Melting example

• Exo or Endo ?• Increasing or decreasing Entropy• Will ice melt spontaneously?

– depends on temperature!!

Page 8: Unit 5 - Chpt 17 - Thermochemistry Part II

ΔSsurroundings

• Heat flow (constant P) = change in enthalpy = ΔH

Page 9: Unit 5 - Chpt 17 - Thermochemistry Part II

Spontaneous Reaction? (Entropy driving force)

Page 10: Unit 5 - Chpt 17 - Thermochemistry Part II

Thermochem Relationships

• Entropy

ΔSuniv = ΔSsys + ΔSsurr

ΔSsurr = - ΔH / T

• Free Energy, G

G = H - TS at constant T

ΔG = ΔH - TΔS

ΔSuniv = - ΔG / T at constant T & P

Page 11: Unit 5 - Chpt 17 - Thermochemistry Part II

Freezing & Melting conditions

• Melting point, boiling point are equilibrium between states ΔSuniv = 0 and thus ΔG = 0

• So ΔGo = ΔHo - TΔSo = 0o means each substance in its standard state.

• Given enthalpy and entropy can calculate the boiling point or freezing pt.

Page 12: Unit 5 - Chpt 17 - Thermochemistry Part II

Exercise 1

The value of ΔHvaporization of substance X is 45.7 kJ/mol, and its normal boiling point is 72.5°C.

Calculate ΔS, ΔSsurr, and ΔG for the vaporization of one mole of this substance at 72.5°C and 1 atm.

ΔS = 132 J/K·mol

ΔSsurr = -132 J/K·molΔG = 0 kJ/mol

Page 13: Unit 5 - Chpt 17 - Thermochemistry Part II

Third Law of Thermodynamics

• The entropy of a pure perfect crystal (every atom aligned - one possible lowest energy configuration) is zero at absolute zero temperature.

• Entropy increases with temperature• Absolute zero cannot be attained. • 2nd Law prohibits heat can never spontaneously move from a

colder body to a hotter body. So, as a system approaches absolute zero, it will eventually have to draw energy from whatever systems are nearby. It would take an infinite number of steps and infinite energy to attain.

Page 14: Unit 5 - Chpt 17 - Thermochemistry Part II

Spontaneous Reaction, G

Page 15: Unit 5 - Chpt 17 - Thermochemistry Part II

State Functions

• Entropy is a state function.• Standard entropy is defined at 298K and 1

atm. Recall at 0 K S = zero

ΔS°reaction = ΣnpS°products – ΣnrS°reactants

Page 16: Unit 5 - Chpt 17 - Thermochemistry Part II

Exercise 2

Calculate ΔS° for the following reaction:

2Na(s) + 2H2O(l) → 2NaOH(aq) + H2(g)

Given the following information: S° (J/K·mol)

Na(s) 51

H2O(l) 70 NaOH(aq) 50

H2(g) 131ΔS°= –11 J/K

Page 17: Unit 5 - Chpt 17 - Thermochemistry Part II

Concept Check

Consider the following system at equilibrium at 25°C.

PCl3(g) + Cl2(g) PCl5(g) ΔG° = −92.50 kJ

What will happen to the ratio of partial pressure of PCl5 to partial pressure of PCl3 if the temperature is raised? Explain.

The ratio will decrease.

Page 18: Unit 5 - Chpt 17 - Thermochemistry Part II

State Function - Free Energy

• The change in free energy that will occur if the reactants in their standard states are converted to the products in their standard states.

ΔG° = ΔH° – TΔS°

ΔG°reaction = ΣnpG°products – ΣnrG°reactants

Page 19: Unit 5 - Chpt 17 - Thermochemistry Part II

Dependence of G on pressure

G = G° + RT ln(P)G is free energy of a particular gas at current

pressure and G° is at 1 atm.

Which can be expanded for a total reaction as…

ΔG = ΔG° + RT ln(Q)Q is the equilibrium reaction quotient, we still

need ΔG° from the standard free energies

Page 20: Unit 5 - Chpt 17 - Thermochemistry Part II

Exercise 3 (example 17.13)

Calculate ΔG at 25oC for the reaction with CO at 5.0atm and H2 at 3.0atm ΔG = ΔG° + RT ln(Q) use thermo data in Appendix 4

CO(g) + 2H2(g) --> CH3OH(l)

ΔGf (CH3OH) = -166kJ ; ΔGf (H2) = 0 ; ΔGf (CO) = -137kJ ΔG° = -29kJ now plug into above equation… T in Kelvin

ln(Q) = 1 / [CO]x[H2]2 = 1/45 = 2.2x10-2

ΔG = -38kJ/mol of reaction

Page 21: Unit 5 - Chpt 17 - Thermochemistry Part II

G and Equilibrium

• The equilibrium point occurs at the lowest value of free energy available to the reaction system.

• At equilibrium ΔG = 0 and Q becomes K

ΔG° = - RT ln(K)

Page 22: Unit 5 - Chpt 17 - Thermochemistry Part II

G illustrationA system can achieve the lowest possible free energy by going to equilibrium, not by going to completion.

Page 23: Unit 5 - Chpt 17 - Thermochemistry Part II

Change in free energy to reach equilibrium

Page 24: Unit 5 - Chpt 17 - Thermochemistry Part II

Temp dependence of K

ΔG° = - RT ln(K) combining with

ΔG° = ΔH° – T ΔS°

ln(K) = - ΔH° ( 1 ) + ΔS°

R ( T ) R

Plotting ln(K) vs 1/T gives slope and intercept of enthalpy and entropy

Page 25: Unit 5 - Chpt 17 - Thermochemistry Part II

Qualitatitive : ΔG° and K

• Qualitative Relationship Between the Change in Standard Free Energy and the Equilibrium Constant for a Given Reaction

Page 26: Unit 5 - Chpt 17 - Thermochemistry Part II

Free Energy and Work

• Maximum possible useful work obtainable from a process at constant temperature and pressure is equal to the change in free energy.

wmax = ΔG

Page 27: Unit 5 - Chpt 17 - Thermochemistry Part II

Reversible car battery charge

Page 28: Unit 5 - Chpt 17 - Thermochemistry Part II

G and Work ramifications

• Achieving the maximum work available from a spontaneous process can occur only via a hypothetical pathway. Any real pathway wastes energy.

• All real processes are irreversible.

• First law: You can’t win, you can only break even.

• Second law: You can’t break even.