Entropy, S Natural processes have a preferred direction of progress, systems tend to progress in the direction of increasing entropy Entropy = a measure of the number of ways in which a system may be arranged = a measure of accessible energy levels = a measure of thermal effects of reversible processes Reversible processes = a small change in conditions could reverse the direction Irreversible processes 1 Spontaneous Processes Proceed in a given direction without being driven by an outside source of energy Increase entropy S of Universe Proceed in a direction towards states with highest probabilities Lead to disipitation of energy 2 Spontaneous Processes Expansion of gas Heat transfer AS = R In Vfin/Vinit AS = Cp ln x2/Ti (1 mol of ideal gas) Second Law of Thermodynamics Entropy of universe increases Spontaneous processes increase entropy of universe ASuniv = ASsyst + ASsurr ASuniv > 0 Spontaneous processes ASuniv < 0 Process does not proceed in given direction AS j = 0 Equilibrium To establish spontaneity of a process, we need to know ASsyst and AS surr Third Law of Thermodynamics Entropy of ideal crystal at 0 K equlas zero • ideal crystal does not exist • 0 K cannot be attained Reference state - perfect ordering - motions, vibrations, rotations ceased S = kln W W = number of microstates of a system AtOK W=1,S = 0 Boltzmann Equation S = kln W k = R/NA = 1.38066 1023J K1 Ludwig Edward Boltzmann W = number of microstates of a system It is possible to establish value of S for a given state (in contrast to H or U) On October 5,1906 committed suicide in Duinu by Trieste Boltzmann Equation T = 0 Winit = 1 S = 0 k = Boltzmann constant = 1.3807 10~23 J K~1 W = number of microstates of a system Wfin = ? In WB = S/k = 41 /1.3807 10"23 = 1024 Standard Entropy S° = Standard molar entropy of a substance látky at 298 K and 1 bar (increase of S on heating a substance from 0 K to 298 K) S° = AS = S (298 K) - S (0 K) J moh1 K"1 Standard Entropies S° at 298 K and 1 bar Substance S°, J K-1 mol1 Substance S°, J K"1 mol1 S8(g) 431 H20 (g) 189 SF6(g) 292 H20 (I) 70 02(g) 205 H20 (s) 41 C02(g) 248 CaC03(s) 93 CO(g) 198 CaO(s) 40 H2 (g) 131 Sn (s) white 52 CH3OH (g) 240 Sn (s) gray 44 CH3OH (I) 127 C(s) graphite 6 C2H5OH (I) 161 C(s) diamond 2 10 Standard Entropies S° Dissolution Substance S°, J K1 moM CH3OH (I) CH3OH (aq) NH4CI (s) NH4CI (aq) 127 133 168 12 Standard Entropies S° Molecular mass, number of atoms in a molecule, number of vibrations and rotations Substance f2 (g) ci2 (g) Br2 (g) i2(g) S°, J K1 mo I1 203 223 Heavy molecules - energy levels close spaced, more available states 13 Standard Entropies S° Substance S°, J K1 mol" Chemical composition More complicated molecules NaCI (s) MgCI2 (s) AICI3 (s) 74 90 167 14 Standard Entropies S° Reaction Entropy AS0 = y n S° - Y n S° r prod prod react react Products - Reactants CH4(g) + 2 02(g) -> C02(g) + 2 H20(1) AS0 = [2(69.9) + 213.6] - [182.6 + 2(205.0)] = -242.8 J K AS°r < 0 for reactions: Formation of solids or liquids from gases Total number of moles of gases decresas AS°r > 0 for reactions: Formation of gases from solids or liquids Total number of moles of gases incresas Second Law of Thermodynamics Entropy of universe increases Spontaneous processes increase entropy of universe ASuniv = ASsyst + ASsurr ASuniv > 0 Spontaneous processes ASuniv < 0 Process does not proceed in given direction AS j = 0 Equilibrium To establish spontaneity of a process, we need to know ASsyst and AS surr Heat Exchange between System and Surroundings ■V At p = const ■fcg^^ Heat (surr) = - AH (system) I Given off (+) Lost (-) Removed (—) Absorbed (+) We can establish AS. AH < 0 exo > 0 endo AS surr > 0 incr At 298 K Sb406(s) + 6C(s) -> 4Sb(s) + 6C02(g) AH = 778 kj ASL1PP = -AH/T = -778 kj / 298 K = -2.6 kj K1 (aj_lb)_IS^Ml Transfer of the same amount of heat at lower temperature increases relatively more entropy of surroundings - cold surroundings are more ordered and then more disturbs Reaction Entropy 2Fe(s) + 3H20(g) -> Fe203(s) + 3H2(g) AS°r = [S°(Fe203(s) + 3S°H2(g)] - [2S°Fe(s) + 3S°H20(g)] AS° = -141.5 J K1 Is this reaction spontaneous at 298 K, is AS°univ > 0? ASuniv _ ASsyst + ASsurr AS°r = AS°syst =-141.5 J K-1 Reaction Spontaneity AS0surr = -AH°syst/T = -AH°r/T AH° = AH°f(Fe203(s)) + 3AH°f(H2(g)) - 2AH°f(Fe (s)) - 3 AH°f(H20(g)) = -100 kJ AS°surr = - AH°syst/T = 336 J K' AS univ - AS syst + AS surr = -141.5 + 336= 194.0 J K-1 Reaction is spontaneous at 298 K, AS°univ > 0 Entropy of Phase Transitions H20(l) ±5 H20(g) at 373 K H20(s) t; H20(l) at 273 K 23 Entropy of Phase Transitions H20(l) ±5 H20(g) pri 373 K Phase Transitions are equilibrium processes at which AS°univ = 0 AS°syst = S°(H20(g)) - S°(H20(l)) = 195.9 J K"1-86.6 J K"1 = 109.1 JK-1 AS°surr = -AHvap/ T = -40.7 kJ/373 K = -109.1 J K1 AS°univ = AS°syst + AS°surr = 0 25 Spontaneous Processes and Gibbs Energy Reaction is spontaneous when ASuniv > 0 ASUniv - ASsyst + ASsurr - ASsyst AHsyst/T > 0 Multiply by - T AH - TASsyst < 0 Multiply by -1 reverse unequal. AG ■ Gibbs Free Energy (= - TASuniv) AG = AH^, - TASs;sl When AG is negative, reaction is spontaneous Gibbs Free Energy 1. AG is a state function 2. AG° Gibbs Free Energy at standard cond. -298 K -1 bar for gases -1 mol I-1 concentration 3. AG° tabulated 1/202 (g) + N2(g) ^ N20 (g) AG°f(N20) = 104.18 kJ moh1 Reactants are more stabile than products Kinetic factors of N20 stability 27 Standard Gibbs Free Energy of Formation AG°f calculated from AH°f and S° C(graphite) + 02(g) S C02(g) AH°f = AHr° = - 393.5 kJ mol1 AS° = S° (C02(g)) - S° (C(graphite)) - S° (02(g)) AS° = 213.60 - 5.74 - 205.00 = 2.86 J K 1 mol1 AG°f = AH°f-TAS°f AG°f = -393.5 - (298)(2.86) = - 394.360 J K 1 mol1 28 Standard Gibbs Free Energy of Formation (at 25 °C) AG°f Substance AG °„ kJ moľ1 NH3 -16.45 C02 - 394.4 N02 + 51.3 H20 (g) - 228.6 H20 (1) - 237.1 C6H6 + 124.3 C2H5OH -174.8 AgCI -109.8 CaC03 - 1128.8 29 AG°r Calculated from AGf° AG°r = 2 nprod AG°f (prod) - 2 nreact AG°f (react) aA + bB ^ cC + dD AG0 = cAG°f (C ) + dAG°f (D) - aAG°f (A) - bAG°f (B) 3NO(g) ±5 N20(g) + N02(g) AG0 = ? AG0 = AG°f(N20)+ AG°f(N02)-3AG°f(NO) AG°r = 104.18 + 51.29 - 3(86.55) = -104 kJ mol1 Influence of Temperature on AG0 AG0 = AH0 - T AS0 AH0 + AS0 + AG0 Negative at high T AH0 + AS0 - AG0 Positive at all T AH0 - AS0 + AG0 Negative at all T AH0 - AS0 - AG0 Negative at low T 31 Chemical Equilibria A In laboratory NaXO* + CaCU CaCCX + 2 NaCi Natron on banks of salt lakes in Egypt CaCCX + 2 NaCI NaXCX + CaCU C. L. Berthollet A ( . . ,a-,ac a An excess of a product can reverse the (1748-1822) r u i *■ v ' course of chemical reaction Reversibile reaction Na2C03 + CaCI2 ^ CaCO, + 2 NaCI L Reaction Quotient Q Unequilibrium concentrations powered to stoichiometric coefficients Reversibile rea [A] = [B] = 1 M [C] = [D] = 0 [A] = [B] = 0 [C] = [D] = 1 M Q - Reaction At the start of reaction: quotient Q = 0/1 0 How far a reaction proceeded from A complete reaction: reactants to products Q _ 1/0 ^ (for a = b = c = d = 1) Chemical Composition and AG One of the most important equations in chemistry ! AG = AG0 + RT InQ Q = Reaction quotient 3NO(g) ±5 N20(g) + N02(g) AG0 = -104 kJ mol1 NO = 0.3 atm ; N70 = 2 atm ; NO, = 1 atm Which direction ? AG = AG0 + RT InQ = -104.0 + (8.314 J K 1 mol1)(298 K) In (74.1) AG = - 93.3 kJ mol-1 Reaction is spontaneous to the right more NO decomposes to products 34 aA + bB ±5 cC + dD Pure rcac rants Chemical Composition and AG AG = AG°r + RT InQ Direction of spontaneous reaction AG! AG°r < 0 Pure products AG 1 Pure reactants Pure products T H a AG0 Pure reactants Q = K At equilibrium AG = 0 AG0 and Equilibrium Constant K AG = AG0 + RT InQ At equilibrium AG = 0 and Q = K AG0 = - RT InK II -— aA + bB ^ cC + dD Reaction Quotient Q and Equilibrium Constant K Q = K. System at equilibrium, no change. Q > K. Concentrations of products are larger then equilibrium concentrations. A part of the products must convert back to reactants to attain equilibrium. Reaction shift to the left. Q < K. Concentrations of reactants are larger then equilibrium concentrations. A part of the reactants must react to products to attain equilibrium. Reaction shift to the right. 37 AG0 and Equilibrium Constant K 3NO(g) ±5 N2Q(g) + NQ2(g) AG0 = -104 kJ mol1 ■ k [no2][n2o\\ 38 AG0 = - RT InK AG0 K At equilibrium (AG = 0) <0 > 1 More products >0 < 1 More reactants = 0 = 1 Equilibrium Constant K K is a function only of temperature Pure phases (I, s) do not influence equilibrium Concentration of solvent is not considered K is dimensionless Concentrations related to standard state 1 M 40 Guldberg-Waage Law 1864 Law of mass action aA + bB ±5 cC + dD Cato Maximilian Guldberg (1836-1902) Peter Waage (1833-1900) 41 Guldberg-Waage Law cC + dD ±5 aA + bB Reverse reaction, Knew = 1/ K ncC + ndD ±z naA + nbB Multiply equation by a constant Knew = (K)n Sum of chemical equations Knew = K1 X K2 42 Guldberg-Waage Law 2 N02 i=» 2 NO + 02 Kj 2 S02 + 02 ^ 2 S03 K2 N02 + S02 i+ NO + S03 K3 = ? K3 = (Kx x K2)1/2 = a/Kj x K2 43 Attaining Chemical Equilibrium H2 + l2 ^2 HI 2 HI -> H2 + l2 concentration H2 + 12 -> 2 HI _ 2HI^H2 + 2 HI 0 ^2, 12 equilibrium ^ state \~^2/ '2 equilibrium ^tate time -> time -> 1 1 Equilibrium concentrations 1 Equilibrium concentrations LeChatelier's Principle Reversibile reactions If a chemical system at equilibrium experiences a change in concentration, temperature, volume, or partial pressure, then the equilibrium shifts to counteract the imposed change and a new equilibrium is established. Henri LeChatelier (1850-1936) . Addition of H time Concentrations K is const. C02 (g) + H2 (g) i; H20 (g) + CO (g) Trapping water, shift to right NaCI (s) + H2S04(l) ±5 Na2S04(s) + HCI (g)f Gaseous HCI escapes, shift to right H2(g) + l2(g)^2HI(g) Addition of inert N2, does not take part in reaction, no change in number of moles, no shift 46 Transfer of Oxygen and C02 hemoglobin Fe2+ highspin ^ oxyhemoglobin Fe2+ lowspin 02-hemoglobin ±+ hemoglobin ^ CO-hemoglobin H20 + C02 + C032- tř 2HCO3- 47 Pressure Reactions with changing number of moles of gases 2 N02(g) ^ N204(g) Ang = (nprod " nreact) = 1 - 2 = -1 V halved, p 2x bigger Q = 72 Kp M____ Increased pressure shifts reaction to the right compress shift New equilibrium 48 Pressure m ■ N2(g) + 3 H2(g) ±5 2 NH3(g) AH = -92 kJ moh1 j V • the reaction is exothermic \ • decreasing number of moles of gases * Fritz Haber According to LeChatelier, the yield will be at (i868-1934) maximum at high pressure and low Mn . _ ,n,0 a K NP in Chemistry 1918 temperature At low temperature, the reaction is slow uses Fe catalyst to speed up Conditions 20-100 MPa and 400-600 °C wmfi i/ Pressure K is con H2 P NH3 N2(g) + 3 H2(g) ±5 2 NH3(g) 50 Equilibrium Constant K pV=nRT p = (n/V)RT=cRT p = Pj + p2 + p3 +.....Partial pressures N2(g) + 3 H2(g) ±5 2 NH3(g) „ [NH3]2 51 Equilibrium Constant K jA + kB ±5 IC + mD K = Kc (RT)An A/7 = (/ + m) - (j + k) (c<2 x i?r)i(cD x j?rr C*V)(Jfc*) Heterogeneous Equilibria CaC03(s) ±5 CaO(s) + C02(g) K = [C02][CaO] / [CaC03] = [C02] = p(C02) Activity (concentration) of pure liquids and solids is constant and does not appear in K. [CaO] = [CaC03] = const. Addition does not change K 53 Heterogeneous Equilibria 2H20(/) ±5 2H2(g) + 02(g) K=[H2]2[02] Kp = p2(H2)p(02) 2H20(g) ±5 m2(g) + 02(g) K = [H2]2[02] / [H20]2 Kv = p2(H2) p(02) / p2(H20) Temperature K changes with Compare K at T1 and T2 (K-, and K2) van't Hoff equation 55 Temperature cooling heating 2 N02 (g) ±5 N204 (g) AH° = - 63 kJ mor Exothermic reactions shift to right - T2 < T, on cooling = K incr., K2 > Heat is a product in exothermic reaction 2N02(g) ^N204(g) + Q Equilibria in Exothermic Reactions N2(g) + 3 H2(g) ^ 2 NH3(g) AH° = - 92 kJ moM Yield decreases with increasing T Temperature CaC03(s) ±5 CaO(s) + C02(g) AH° = 556 kJ moh1 Endothermic reactions shift to right on heating T2>T1 K incr, K2 > ^ , K = p(C02) Heat is a reactant in endothermic reactions CaC03(s) + Q ±5 CaO(s) + C02(g) Equilibrium Concentrations H2(0) + F2(fli) *? 2HF(g) K= 1.15 102 = [HF]2/[H2][F2] [H2]0=1.00/W [F2]0=2.00M [HF]0 = 0 Initial Change Equilibrium H2(flf) 1.00 -x 1.00-x F2(0) 2.00 - x 2.00-x 2HF(^) 0 +2x 2x K = 1.15 102 = [HF]2 / [H2][F2] = (2x)2 / (1.00 - x)(2.00 - x) 59 Equilibrium Concentrations x, 2 = [- b + (b2 - 4ac),/2] / 2a x1 = 2.14 mol h1 a x2 = 0.968 mol h1 Use x2= 0.968 mol h1 [H2]= 1.000 M- 0.968 yW= 3.2 10"2yW [F2] = 2.000 yW-0.968 yW= 1.032 M [HF] = 2 (0.968 /W) = 1.936 M 60