CHAPTER Chemical Equilibrium 4
ow we arrive at the point where real chemistry begins. Chemical thermo- Thermodynamic background dynamics is used to predict whether a mixture of reactants has a sponta- 4.1 The reaction Gibbs energy neous tendency to change into products, to predict the composition of the N 4.2 The variation of rG with reaction mixture at equilibrium, and to predict how that composition will be mod- composition ified by changing the conditions. In biology, life is the avoidance of equilibrium, 4.3 Reactions at equilibrium and the attainment of equilibrium is death, but knowing whether equilibrium lies CASE STUDY 4.1: Binding of in favor of reactants or products under certain conditions is a good indication of oxygen to myoglobin and the feasibility of a biochemical reaction. Indeed, the material we cover in this chap- hemoglobin ter is of crucial importance for understanding the mechanisms of oxygen transport 4.4 The standard reaction in blood, metabolism, and all the processes going on inside organisms. Gibbs energy There is one word of warning that is essential to remember: thermodynamics is silent about the rates of reaction. All it can do is to identify whether a particular re- The response of equilibria to the conditions action mixture has a tendency to form products; it cannot say whether that ten- dency will ever be realized. We explore what determines the rates of chemical re- 4.5 The presence of a catalyst actions in Chapters 6 through 8. 4.6 The effect of temperature Coupled reactions in Thermodynamic background bioenergetics 4.7 The function of adenosine The thermodynamic criterion for spontaneous change at constant temperature and triphosphate pressure is G 0. The principal idea behind this chapter, therefore, is that, at CASE STUDY 4.2: The constant temperature and pressure, a reaction mixture tends to adjust its composition un- biosynthesis of proteins til its Gibbs energy is a minimum. If the Gibbs energy of a mixture varies as shown 4.8 The oxidation of glucose in Fig. 4.1a, very little of the reactants convert into products before G has reached its minimum value, and the reaction “does not go.” If G varies as shown in Proton transfer equilibria Fig. 4.1c, then a high proportion of products must form before G reaches its min- 4.9 Brønsted-Lowry theory imum and the reaction “goes.” In many cases, the equilibrium mixture contains al- 4.10 Protonation and most no reactants or almost no products. Many reactions have a Gibbs energy that deprotonation varies as shown in Fig. 4.1b, and at equilibrium the reaction mixture contains sub- 4.11 Polyprotic acids stantial amounts of both reactants and products. CASE STUDY 4.3: The fractional composition of a 4.1 The reaction Gibbs energy solution of lysine 4.12 Amphiprotic systems To explore metabolic processes, we need a measure of the driving power of a 4.13 Buffer solutions chemical reaction, and to understand the chemical composition of cells, we need CASE STUDY 4.4: Buffer action to know what those compositions would be if the reactions taking place in them in blood had reached equilibrium. Exercises To keep our ideas in focus, we consider two important processes. One is the iso- merism of glucose-6-phosphate (1, G6P) to fructose-6-phosphate (2, F6P), which is an early step in the anaerobic breakdown of glucose (Section 4.8):
G6P(aq) 0ˆˆˆ9 F6P(aq) (A)
151 152 Chapter 4 • Chemical Equilibrium
2– OPO 3 2– OPO 3 OH O H H O G OH H H HO HO OH H OH
OH (a) (b) (c) H OH H Gibbs energy, Gibbs energy, 1 Glucose-6-phosphate 2 Fructose-6-phosphate
The second is the binding of O2(g) to the protein hemoglobin, Hb, in blood (Case Pure Pure study 4.1): reactants products
Fig. 4.1 The variation of Hb(aq) 4 O2(g) 0ˆˆˆ9 Hb(O2)4(aq) (B) Gibbs energy of a reaction mixture with progress of the These two reactions are specific examples of a general reaction of the form reaction, pure reactants on the left and pure products on the ˆˆ9 right. (a) This reaction “does a A b B 0ˆˆ c C d D (C) not go”: the minimum in the Gibbs energy occurs very close with arbitrary physical states. to the reactants. (b) This First, consider reaction A. Suppose that in a short interval while the reaction reaction reaches equilibrium is in progress, the amount of G6P changes infinitesimally by dn. As a result of with approximately equal this change in amount, the contribution of G6P to the total Gibbs energy of the amounts of reactants and system changes by G6Pdn, where G6P is the chemical potential (the partial mo- products present in the lar Gibbs energy) of G6P in the reaction mixture. In the same interval, the amount mixture. (c) This reaction goes of F6P changes by dn, so its contribution to the total Gibbs energy changes by almost to completion, as the minimum in Gibbs energy lies F6Pdn, where F6P is the chemical potential of F6P. The change in Gibbs en- very close to pure products. ergy of the system is
dG F6Pdn G6Pdn
On dividing through by dn, we obtain the reaction Gibbs energy, rG:
dG G (4.1a) dn F6P G6P r
There are two ways to interpret rG. First, it is the difference of the chemical potentials of the products and reactants at the composition of the reaction mixture. Second, we can think of rG as the derivative of G with respect to n, or the slope of the graph of G plotted against the changing composition of the system (Fig. 4.2). The binding of oxygen to hemoglobin provides a slightly more complicated ex- ample. If the amount of Hb changes by dn, then from the reaction stoichiome- try we know that the change in the amount of O2 will be 4dn and the change in the amount of Hb(O2)4 will be dn. Each change contributes to the change in the total Gibbs energy of the mixture, and the overall change is