CHEMISTRY The Molecular Nature of Matter and Change Third Edition Chapter 20 Lecture Outlines* *See PowerPoint Image Slides for all figures and tables pre-inserted into PowerPoint without notes. 20-1 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Chapter 20 Thermodynamics: Entropy, Free Energy and the Direction of Chemical Reactions 20-2 Thermodynamics: Entropy, Free Energy, and the Direction of Chemical Reactions 20.1 The Second Law of Thermodynamics: Predicting Spontaneous Change 20.2 Calculating the Change in Entropy of a Reaction 20.3 Entropy, Free Energy, and Work 20.4 Free Energy, Equilibrium, and Reaction Direction 20-3 Limitations of the First Law of Thermodynamics Esystem = Ek + Ep DEsystem = heat + work DEsystem = q + w Euniverse = Esystem + Esurroundings DEsystem = -DEsurroundings The total energy-mass of the universe is constant. But, this does not tell us anything about the direction of change in the universe. 20-4 Figure 20.1 A spontaneous endothermic chemical reaction Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. water Ba(OH)2.8H2O(s) + 2NH4NO3(s) Ba2+(aq) + 2NO3-(aq) + 2NH3(aq) + 10H2O(l) DH0rxn = + 62.3 kJ 20-5 The Concept of Entropy (S) Entropy refers to the state of order. A change in order is a change in the number of ways of arranging the particles, and it is a key factor in determining the direction of a spontaneous process. more order solid more order crystal + liquid more order crystal + crystal 20-6 less order liquid gas less order ions in solution less order gases + ions in solution Figure 20.2 20-7 The number of ways to arrange a deck of playing cards Figure 20.3 Spontaneous expansion of a gas stopcock closed 1 atm evacuated stopcock opened 0.5 atm 20-8 0.5 atm 1877 Ludwig Boltzman S = k ln W S = entropy W = number of ways of arranging the components of a system k = Boltzman constant •A system with relatively few equivalent ways to arrange its components (smaller W) has relatively less disorder and low entropy. •A system with many equivalent ways to arrange its components (larger W) has relatively more disorder and high entropy. 2nd law of thermodynamics The universe is going to a higher state of entropy DSuniverse = DSsystem + DSsurroundings > 0 20-9 Figure 20.4 3rd Law of thermodynamics A perfect crystal has zero entropy at a temperature of absolute zero. Ssystem = 0 at 0 K 20-10 Random motion in a crystal Predicting Relative S0 Values of a System 1. Temperature changes S0 increases as the temperature rises. 2. Physical states and phase changes S0 increases as a more ordered phase changes to a less ordered phase. 3. Dissolution of a solid or liquid S0 of a dissolved solid or liquid is usually greater than the S0 of the pure solute. However, the extent depends upon the nature of the solute and solvent. 4. Dissolution of a gas A gas becomes more ordered when it dissolves in a liquid or solid. 5. Atomic size or molecular complexity In similar substances, increases in mass relate directly to entropy. In allotropic substances (e.g. O2 & O3), increases in complexity (e.g. bond flexibility) relate directly to entropy. 20-11 Figure 20.5 20-12 The increase in entropy from solid to liquid to gas Figure 20.6 The entropy change accompanying the dissolution of a salt pure solid MIX pure liquid solution 20-13 Figure 20.7 The small increase in entropy when ethanol dissolves in water Ethanol 20-14 Water Solution of ethanol and water Figure 20.8 The large decrease in entropy when a gas dissolves in a liquid O2 gas 20-15 Figure 20.9 Entropy and vibrational motion NO NO2 20-16 N 2 O4 Sample Problem 20.1: Predicting Relative Entropy Values PROBLEM: Choose the member with the higher entropy in each of the following pairs, and justify your choice [assume constant temperature, except in part (e)]: (a) 1mol of SO2(g) or 1mol of SO3(g) (b) 1mol of CO2(s) or 1mol of CO2(g) (c) 3mol of oxygen gas (O2) or 2mol of ozone gas (O3) (d) 1mol of KBr(s) or 1mol of KBr(aq) (e) Seawater in midwinter at 20C or in midsummer at 230C (f) 1mol of CF4(g) or 1mol of CCl4(g) PLAN: In general less ordered systems have higher entropy than ordered systems and entropy increases with an increase in temperature. SOLUTION: (a) 1mol of SO3(g) - more atoms (d) 1mol of KBr(aq) - solution > solid (b) 1mol of CO2(g) - gas > solid (e) 230C - higher temperature (c) 3mol of O2(g) - larger #mols (f) CCl4 - larger mass 20-17 Sample Problem 20.4: Calculating DG0 from Enthalpy and Entropy Values ( 1of 2) PROBLEM: Potassium chlorate, one of the common oxidizing agents in explosives, fireworks, and matchheads, undergoes a solidstate redox reaction when heated. In this reaction, note that the oxidation number of Cl in the reactant is higher in one of the products and lower in the other (disproportionation): +5 +7 -1 D 4KClO3(s) 3KClO4(s) + KCl(s) Use DH0f and S0 values to calculate DG0sys (DG0rxn) at 250C for this reaction. PLAN: Use Appendix B values for thermodynamic entities; place them into the Gibbs Free Energy equation and solve. SOLUTION: DH0rxn = S mDHf0products - S nDHf0reactants DH0rxn = (3mol)(-432.8kJ/mol) + (1mol)(-436.7kJ/mol) (4mol)(-397.7kJ/mol) DH0rxn = -144kJ 20-18 Sample Problem 20.4: Calculating DG0 from Enthalpy and Entropy Values continued DS0rxn = S mS0products - S nS0reactants DS0rxn = (3mol)(151J/mol*K) + (1mol)(82.6J/mol*K) (4mol)(143.1J/mol*K) DS0rxn = -36.8J/K DG0rxn = DH0rxn - T DS0rxn DG0rxn = -144kJ - (298K)(-36.8J/K)(kJ/103J) DG0rxn = -133kJ 20-19 Sample Problem 20.2: PROBLEM: Calculating the Standard Entropy of Reaction, DS0rxn Calculate DS0rxn for the combustion of 1mol of propane at 250C. C3H8(g) + 5O2(g) 3CO2(g) + 4H2O(l) PLAN: Use summation equations. It is obvious that entropy is being lost because the reaction goes from 6mols of gas to 3mols of gas. SOLUTION: Find standard entropy values in the Appendix or other table. DS = [(3mol)(S0 CO2) + (4mol)(S0 H2O)] - [(1mol)(S0 C3H8) + (5mol)(S0 O2)] DS = [(3mol)(213.7J/mol*K) + (4mol)(69.9J/mol*K)] - [(1mol)(269.9J/mol*K) + (5mol)(205.0J/mol*K)] DS = - 374 J/K 20-20 Figure B20.1 Lavoisier studying human respiration as a form of combustion 20-21 Figure B20.2 20-22 A whole-body calorimeter Figure 20.10 Components of DS0universe for spontaneous reactions DSuniverse = DSsystem + DSsurroundings endothermic exothermic system becomes more disordered system becomes more disordered exothermic system becomes more ordered 20-23 Sample Problem 20.3: PROBLEM: Determining Reaction Spontaneity At 298K, the formation of ammonia has a negative DS0sys; N2(g) + 3H2(g) 2NH3(g) DS0sys = -197J/K Calculate DS0rxn, and state whether the reaction occurs spontaneously at this temperature. PLAN: DS0universe must be > 0 in order for this reaction to be spontaneous, so DS0surroundings must be > 197J/K. To find DS0surr, first find DHsys; DHsys = DHrxn which can be calculated using DH0f values from tables. DS0universe = DS0surr + DS0sys. SOLUTION: DH0rx = [(2mol)(DH0fNH3)] - [(1mol)(DH0fN2) + (3mol)(DH0fH2)] DH0rx = -91.8kJ DS0surr = -DH0sys/T = -(-91.8x103J/298K) = 308J/K DS0universe = DS0surr + DS0sys = 308J/K + (-197J/K) = 111J/K DS0universe > 0 so the reaction is spontaneous. 20-24 Useful Thermodynamic Relationships Different Ways to Calculate DG0rxn 0 = Std conds: 25oC, 1 atm, 1 M solutions (Eqn 1) DG0rxn = DH0rxn - TDS0rxn (Eqn 2) DG0rxn = S mDGf0products - S nDGf0reactants (Eqn 3) DG0 = - RT lnKeq R = 8.314 J/mol.K When not at standard conditions (Eqn 4) DGrxn = DG0rxn + RT ln Q (Q = Reaction Quotient) Use these equations with equation #1 DS0rxn = S mS0products - S nS0reactants DH0rxn = S mDHf0products - S nDHf0reactants 20-25 Sample Problem 20.6: PROBLEM: Determining the Effect of Temperature on DG0 (1 of 2) An important reaction in the production of sulfuric acid is the oxidation of SO2(g) to SO3(g): 2SO2(g) + O2(g) 2SO3(g) At 298K, DG0 = -141.6kJ; DH0 = -198.4kJ; and DS0 = -187.9J/K (a) Use the data to decide if this reaction is spontaneous at 250C, and predict how DG0 will change with increasing T. (b) Assuming DH0 and DS0 are constant with increasing T, is the reaction spontaneous at 900.0C? PLAN: The sign of DG0 tells us whether the reaction is spontaneous and the signs of DH0 and DS0 will be indicative of the T effect. Use the Gibbs free energy equation for part (b). SOLUTION: (a) The reaction is spontaneous at 250C because DG0 is (-). Since DH0 is (-) but DS0 is also (-), DG0 will become less spontaneous as the temperature increases. 20-26 Sample Problem 20.6: Determining the Effect of Temperature on DG0 (2 of 2) continued (b) DG0rxn = DH0rxn - T DS0rxn DG0rxn = -198.4kJ - (1173K)(-187.9J/mol*K)(kJ/103J) DG0rxn = 22.0 kJ; the reaction will be nonspontaneous at 900.0C 20-27 DG and the Work a System Can Do For a spontaneous process, DG is the maximum work obtainable from the system as the process takes place: DG = workmax For a nonspontaneous process, DG is the maximum work that must be done to the system as the process takes place: DG = workmax An example 20-28 Table 20.1 Reaction Spontaneity and the Signs of DH0, DS0, and DG0 DH0 DS0 -TDS0 DG0 - + - - Spontaneous at all T + - + + Nonspontaneous at all T + + - + or - Spontaneous at higher T; nonspontaneous at lower T - - + + or - Spontaneous at lower T; nonspontaneous at higher T 20-29 Description Sample Problem 20.5: PROBLEM: PLAN: Calculating DG0rxn from DG0f Values Use DG0f values to calculate DGrxn for the reaction in Sample Problem 20.4: D 4KClO3(s) 3KClO4(s) + KCl(s) Use the DG summation equation. SOLUTION: DG0rxn = S mDGf0products - S nDGf0reactants DG0rxn = (3mol)(-303.2kJ/mol) + (1mol)(-409.2kJ/mol) - (4mol)(-296.3kJ/mol) DG0rxn = -134kJ 20-30 Figure 20.11 20-31 The effect of temperature on reaction spontaneity The coupling of a nonspontaneous reaction to the hydrolysis of ATP. Glucose-6-phosphate Enzyme: hexose kinase Glucose Enzyme 1st Rxn of Glycolysis catalyzed by Hexose Kinase: Glucose + HPO42- Glucose-6-phosphate + H2O ATP4- + H2O ADP3- + HPO42Glucose + HPO42- Glucose-6-phosphate + H2O Glucose 20-32 + ATP Glucose-6-phosphate + ADP3- DG0 = +13.8 kJ DG0 = -30.5 kJ DG0 = +13.8 kJ DG0 = -16.7 kJ Figure B20.4 20-33 The cycling of metabolic free energy through ATP Figure B20.5 20-34 Why is ATP a high-energy molecule? Free Energy, Equilibrium and Reaction Direction •If Q/K < 1, then ln Q/K < 0; the reaction proceeds to the right (DG < 0) •If Q/K > 1, then ln Q/K > 0; the reaction proceeds to the left (DG > 0) •If Q/K = 1, then ln Q/K = 0; the reaction is at equilibrium (DG = 0) DG = RT ln Q/K = RT lnQ - RT lnK Under standard conditions (1M concentrations, 1atm for gases), Q = 1 and lnQ = 0 so... DG0 = - RT lnK 20-35 Table 20.2 The Relationship Between DG0 and K at 250C DG0(kJ) 100 3x10-18 50 2x10-9 10 2x10-2 1 7x10-1 0 1 Essentially no forward reaction; reverse reaction goes to completion Forward and reverse reactions proceed to same extent 1.5 -10 5x101 -50 6x108 -100 3x1017 -200 1x1035 Forward reaction goes to completion; essentially no reverse reaction REVERSE REACTION 9x10-36 Significance FORWARD REACTION 200 -1 20-36 K Sample Problem 20.7: PROBLEM: Calculating DG at Nonstandard Conditions The oxidation of SO2, which we considered in Sample Problem 20.6 2SO2(g) + O2(g) 2SO3(g) is too slow at 298K 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 298K and at 973K. (DG0298 = -141.6kJ/mol of reaction as written using DH0 and DS0 values at 973K. DG0973 = -12.12kJ/mol of reaction as written.) (b) In experiments to determine the effect of temperature on reaction spontaneity, two sealed containers are filled with 0.500atm of SO2, 0.0100atm of O2, and 0.100atm of SO3 and kept at 250C and at 700.0C. In which direction, if any, will the reaction proceed to reach equilibrium at each temperature? (c) Calculate DG for the system in part (b) at each temperature. PLAN: Use the equations and conditions found on slide 20-37 . Sample Problem 20.7: Calculating DG at Nonstandard Conditions continued (2 of 3) SOLUTION: (a) Calculating K at the two temperatures: DG0 = -RTlnK so K e (DG / RT ) 0 (-141.6kJ/mol)(103J/kJ) At 298, the exponent is -DG0/RT = - = 57.2 (8.314J/mol*K)(298K) K e (DG / RT ) 0 = e57.2 = 7x1024 (-12.12kJ/mol)(103J/kJ) At 973, the exponent is -DG0/RT = 1.50 (8.314J/mol*K)(973K) K e 20-38 (DG / RT ) 0 = e1.50 = 4.5 Calculating DG at Nonstandard Conditions Sample Problem 20.7: continued (3 of 3) pSO32 (b) The value of Q = (pSO2)2(pO2) (0.100)2 = = 4.00 (0.500)2(0.0100) Since Q is < K at both temperatures the reaction will shift right; for 298K there will be a dramatic shift while at 973K the shift will be slight. (c) The nonstandard DG is calculated using DG = DG0 + RTlnQ DG298 = -141.6kJ/mol + (8.314J/mol*K)(kJ/103J)(298K)(ln4.00) DG298 = -138.2kJ/mol DG973 = -12.12kJ/mol + (8.314J/mol*K)(kJ/103J)(973K)(ln4.00) DG298 = -0.9kJ/mol 20-39 Figure 20.12 The relation between free energy and the extent of reaction DG0 < 0 K >1 20-40 DG0 > 0 K <1 Useful Thermodynamic Relationships Different Ways to Calculate DGrxn (Eqn 1) DG0rxn = DH0rxn - TDS0rxn (Eqn 2) DG0rxn = S mDGf0products - S nDGf0reactants (Eqn 3) DG0 = - RT lnKeq (Eqn 4) DG = DG0 + RT lnQ R = 8.314 J/mol.K Q = Rxn Quotient Use these with equation #1 DS0rxn = S mS0products - S nS0reactants DH0rxn = S mDHf0products - S nDHf0reactants 20-41