Entropy and Free Energy How to predict if a reaction can occur, given enough time? THERMODYNAMICS How to predict if a reaction can occur at a reasonable rate? KINETICS Copyright © 1999 by Harcourt Brace & Company All rights reserved. Requests for permission to make copies of any part of the work should be mailed to: Permissions Department, Harcourt Brace & Company, 6277 Sea Harbor Drive, Orlando, Florida Thermodynamics • Is the state of a chemical system such that a rearrangement of its atoms and molecules would decrease the energy of the system? • If yes, system is favored to react — a product-favored system. • Most product-favored reactions are exothermic. • Often referred to as spontaneous reactions. • Spontaneous does not imply anything about time for reaction to occur. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Kinetics Diamond is thermodynamically favored to convert to graphite, but not kinetically favored. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Kinetics Diamond is thermodynamically favored to convert to graphite, but not kinetically favored. Paper burns — a product-favored reaction. Also kinetically favored once reaction is begun. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Product-Favored Reactions In general, productfavored reactions are exothermic. Fe2O3(s) + 2 Al(s) ---> 2 Fe(s) + Al2O3(s) DH = - 848 kJ Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Product-Favored Reactions But many spontaneous reactions or processes are endothermic or even have DH = 0. NH4NO3(s) + heat ---> NH4NO3(aq) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Entropy, S One property common to product-favored processes is that the final state is more DISORDERED or RANDOM than the original. Spontaneity is related to an increase in randomness. The thermodynamic property related to randomness is ENTROPY, S. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Reaction of K with water The entropy of liquid water is greater than the entropy of solid water (ice) at 0 C. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Directionality of Reactions How probable is it that reactant molecules will react? PROBABILITY suggests that a product-favored reaction will result in the dispersal of energy or of matter or both. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Directionality of Reactions Probability suggests that a productfavored reaction will result in the dispersal of energy or of matter or both. Matter Dispersal Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Directionality of Reactions Probability suggests that a productfavored reaction will result in the dispersal of energy or of matter or both. Matter Dispersal Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Directionality of Reactions Probability suggests that a productfavored reaction will result in the dispersal of energy or of matter or both. Energy Dispersal Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Directionality of Reactions Probability suggests that a productfavored reaction will result in the dispersal of energy or of matter or both. Energy Dispersal Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Directionality of Reactions — Energy Dispersal Exothermic reactions involve a release of stored chemical potential energy to the surroundings. The stored potential energy starts out in a few molecules but is finally dispersed over a great many molecules. The final state—with energy dispersed—is more probable and makes a reaction product-favored. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Entropy, S S (gases) > S (liquids) > S (solids) So (J/K•mol) H2O(liq) 69.91 H2O(gas) 188.8 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Entropy, S Entropy of a substance increases with temperature. Molecular motions of heptane, C7H16 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Molecular motions of heptane at different temps. Entropy, S Increase in molecular complexity generally leads to increase in S. So (J/K•mol) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved CH4 248.2 C2H6 336.1 C3H8 419.4 Entropy, S Entropies of ionic solids depend on coulombic attractions. So (J/K•mol) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved MgO 26.9 NaF 51.5 Entropy, S Entropy usually increases when a pure liquid or solid dissolves in a solvent. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Entropy Changes for Phase Changes For a phase change, DS = q/T where q = heat transferred in phase change For H2O (liq) ---> H2O(g) DH = q = +40,700 J/mol Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Entropy Changes for Phase Changes For a phase change, DS = q/T where q = heat transferred in phase change For H2O (liq) ---> H2O(g) DH = q = +40,700 J/mol q 40,700 J/mol DS = = = + 109 J/K • mol T 373.15 K Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Calculating DS for a Reaction D So = So (products) - So (reactants) Consider 2 H2(g) + O2(g) ---> 2 H2O(liq) DSo = 2 So (H2O) - [2 So (H2) + So (O2)] DSo = 2 mol (69.9 J/K•mol) [2 mol (130.7 J/K•mol) + 1 mol (205.3 J/K•mol)] DSo = -326.9 J/K Note that there is a decrease in S because 3 mol of gas give 2 mol of liquid. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2nd Law of Thermodynamics A reaction is spontaneous (productfavored) if ²S for the universe is positive. DSuniverse = DSsystem + DSsurroundings DSuniverse > 0 for product-favored process First calc. entropy created by matter dispersal (DSsystem) Next, calc. entropy created by energy dispersal (DSsurround) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2nd Law of Thermodynamics Dissolving NH4NO3 in water—an entropy driven process. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2nd Law of Thermodynamics 2 H2(g) + O2(g) ---> 2 H2O(liq) DSosystem = -326.9 J/K Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2nd Law of Thermodynamics 2 H2(g) + O2(g) ---> 2 H2O(liq) DSosystem = -326.9 J/K DS o surroundi ngs Copyright (c) 1999 by Harcourt Brace & Company All rights reserved qsurroundi ngs -DH system = = T T 2nd Law of Thermodynamics 2 H2(g) + O2(g) ---> 2 H2O(liq) DSosystem = -326.9 J/K DS o surroundi ngs qsurroundi ngs -DH system = = T T Can calc. that DHorxn = DHosystem = -571.7 kJ Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2nd Law of Thermodynamics 2 H2(g) + O2(g) ---> 2 H2O(liq) DSosystem = -326.9 J/K DS o surroundi ngs qsurroundi ngs -DH system = = T T Can calc. that DHorxn = DHosystem = -571.7 kJ DS o surroundi ngs Copyright (c) 1999 by Harcourt Brace & Company All rights reserved - (-571.7 kJ)(1000 J/kJ) = 298.15 K 2nd Law of Thermodynamics 2 H2(g) + O2(g) ---> 2 H2O(liq) DSosystem = -326.9 J/K DS o surroundi ngs qsurroundi ngs -DH system = = T T Can calc. that DHorxn = DHosystem = -571.7 kJ DS o surroundi ngs - (-571.7 kJ)(1000 J/kJ) = 298.15 K DSosurroundings = +1917 J/K Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2nd Law of Thermodynamics 2 H2(g) + O2(g) ---> 2 H2O(liq) DSosystem = -326.9 J/K DSosurroundings = +1917 J/K DSouniverse = +1590. J/K The entropy of the universe is increasing, so the reaction is productfavored. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved 2nd Law of Thermodynamics 2 H2(g) + O2(g) ---> 2 H2O(liq) DSosystem = -326.9 J/K DSosurroundings = +1917 J/K DSouniverse = +1590. J/K The entropy of the universe is increasing, so the reaction is productfavored. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G ²Suniv = ²Ssurr + ²Ssys Copyright © 1999 by Harcourt Brace & Company All rights reserved. Requests for permission to make copies of any part of the work should be mailed to: Permissions Department, Harcourt Brace & Company, 6277 Sea Harbor Drive, Orlando, Florida Gibbs Free Energy, G ²Suniv = ²Ssurr + ²Ssys DHsys DSuniv = + DSsys T Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G ²Suniv = ²Ssurr + ²Ssys DHsys DSuniv = + DSsys T Multiply through by -T Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G D Suniv = D Ssurr + D Ssys D Hsys + D Ssys DSuniv = T Multiply through by -T -T D Suniv = D Hsys - T D Ssys Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G D Suniv = D Ssurr + D Ssys DHsys DSuniv = + DSsys T Multiply through by -T -T D Suniv = D Hsys - T D Ssys -T D Suniv = change in Gibbs free energy for the system = D Gsystem Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G DSuniv = DSsurr + DSsys D Hsys + D Ssys DSuniv = T Multiply through by -T -TDSuniv = DHsys - TDSsys -TDSuniv = change in Gibbs free energy for the system = DGsystem Under standard conditions — DGo = DHo - TDSo Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G o DG = o DH - T o DS Gibbs free energy change = total energy change for system - energy lost in disordering the system If reaction is exothermic (DHo negative) and entropy increases (DSo is +), then DGo must be negative and reaction product-favored. If reaction is endothermic (DHo is +), and entropy decreases (DSo is -), then DGo must be + and reaction is reactant-favored. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G o DG = o DH o TDS - DHo DSo DGo Reaction exo(-) increase(+) - Prod-favored endo(+) decrease(-) + React-favored exo(-) decrease(-) ? T dependent endo(+) increase(+) ? T dependent Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G o DG = o DH - o TDS Two methods of calculating DGo Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G o DG = o DH - o TDS Two methods of calculating DGo a) Determine DHorxn and DSorxn and use GIbbs equation. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G o DG = o DH - o TDS Two methods of calculating DGo a) Determine DHorxn and DSorxn and use GIbbs equation. b) Use tabulated values of free energies of formation, DGfo. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Gibbs Free Energy, G o DG = o DH - o TDS Two methods of calculating DGo a) Determine DHorxn and DSorxn and use GIbbs equation. b) Use tabulated values of free energies of formation, DGfo. ²Gorxn = ²Gfo (products) - ²Gfo (reactants) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Calculating D o G rxn Combustion of acetylene C2H2(g) + 5/2 O2(g) --> 2 CO2(g) + H2O(g) Use enthalpies of formation to calculate DHorxn = -1238 kJ Use standard molar entropies to calculate DSorxn = -97.4 J/K or -0.0974 kJ/K DGorxn = -1238 kJ - (298 K)(-0.0974 J/K) = -1209 kJ Reaction is product-favored in spite of negative DSorxn. Reaction is “enthalpy driven” Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Calculating D o G rxn NH4NO3(s) + heat ---> NH4NO3(aq) Is the dissolution of ammonium nitrate productfavored? If so, is it enthalpy- or entropy-driven? Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Calculating D o G rxn NH4NO3(s) + heat ---> NH4NO3(aq) From tables of thermodynamic data we find DHorxn = +25.7 kJ DSorxn = +108.7 J/K or +0.1087 kJ/K DGorxn = +25.7 kJ - (298 K)(+0.1087 J/K) = -6.7 kJ Reaction is product-favored in spite of negative DHorxn. Reaction is “entropy driven” Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Calculating D DGorxn = ²Gfo (products) - DGfo (reactants) o G rxn Combustion of carbon C(graphite) + O2(g) --> CO2(g) DGorxn = DGfo(CO2) - [DGfo(graph) + DGfo(O2)] DGorxn = -394.4 kJ - [ 0 + 0] Note that free energy of formation of an element in its standard state is 0. DGorxn = -394.4 kJ Reaction is product-favored as expected. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Free Energy and Temperature 2 Fe2O3(s) + 3 C(s) ---> 4 Fe(s) + 3 CO2(g) DHorxn = +467.9 kJ DSorxn = +560.3 J/K DGorxn = +300.8 kJ Reaction is reactant-favored at 298 K At what T does DGorxn just change from being (+) to being (-)? When DGorxn = 0 = DHorxn - TDSorxn Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Free Energy and Temperature 2 Fe2O3(s) + 3 C(s) ---> 4 Fe(s) + 3 CO2(g) DHorxn = +467.9 kJ DSorxn = +560.3 J/K DGorxn = +300.8 kJ Reaction is reactant-favored at 298 K At what T does DGorxn just change from being (+) to being (-)? When DGorxn = 0 = DHorxn - TDSorxn DHrxn 467.9 kJ T = = = 835.1 K DSrxn 0.5603 kJ/K Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq Keq is related to reaction favorability. When DGorxn < 0, reaction moves energetically “downhill” ²Gorxn is the change in free energy as reactants convert completely to products. But systems often reach a state of equilibrium in which reactants have not converted completely to products. In this case DGrxn is < DGorxn , so state with both reactants and products present is more stable than complete conversion. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq Product-favored reaction. 2 NO2 ---> N2O4 DGorxn = -4.8 kJ Here DGrxn is less than DGorxn , so the state with both reactants and products present is more stable than complete conversion. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq Reactant-favored reaction. N2O4 --->2 NO2 DGorxn = +4.8 kJ Here DGorxn is greater than DGrxn , so the state with both reactants and products present is more stable than complete conversion. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq Keq is related to reaction favorability and so to DGorxn. The larger the value of DGorxn the larger the value of K. o DG rxn = - RT lnK where R = 8.31 J/K•mol Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq DGorxn = - RT lnK Calculate K for the reaction N2O4 --->2 NO2 DGorxn = +4.8 kJ Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq DGorxn = - RT lnK Calculate K for the reaction N2O4 --->2 NO2 DGorxn = +4.8 kJ DGorxn = +4800 J = - (8.31 J/K)(298 K) ln K Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq DGorxn = - RT lnK Calculate K for the reaction N2O4 --->2 NO2 DGorxn = +4.8 kJ DGorxn = +4800 J = - (8.31 J/K)(298 K) ln K 4800 J lnK = = - 1.94 (8.31 J/K)(298K) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq DGorxn = - RT lnK Calculate K for the reaction N2O4 --->2 NO2 DGorxn = +4.8 kJ DGorxn = +4800 J = - (8.31 J/K)(298 K) ln K 4800 J lnK = = - 1.94 (8.31 J/K)(298K) K = 0.14 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Thermodynamics and Keq DGorxn = - RT lnK Calculate K for the reaction N2O4 --->2 NO2 DGorxn = +4.8 kJ DGorxn = +4800 J = - (8.31 J/K)(298 K) ln K 4800 J lnK = = - 1.94 (8.31 J/K)(298K) K = 0.14 When DGorxn > 0, then K < 1 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved