CHM 3410 - Physical Chemistry I Chapter 5 - Supplementary Material 1. Chemical potential for ideal and non-ideal liquids and gases Chemical potential plays a central role in thermodynamics. Chemical potential is defined as J = (G/nJ)p,T,n’ (1.1) where n' indicates that the moles of all substances except the J th substance are held constant. Note that for a pure substance the chemical potential is equal to the molar Gibbs free energy. By analogy, the chemical potential for a mixture is sometimes called the partial molar Gibbs free energy. For chemical reactions and other processes we are usually only interested in changes in free energy. Therefore, in working with substances, whether real or ideal, we choose convenient reference states, and then express the chemical potential in terms of the value found for the reference state. Expressions for the chemical potential for a number of common situations are given below. Gases General expression J = J + RT ln fJ/p = J + RT ln fJ (division by p implied) Reference state J, the chemical potential at standard pressure (usually taken as 1 bar or 1 atm) and assuming ideal gas behavior. This therefore represents a hypothetical state for the gas. Fugacity fJ, the "effective pressure" of the gas. Fugacity coefficient J, defined by the expression fJ = J pJ, where pJ is the partial pressure of the gas. For a pure gas J can be found from the relationship ln J = 0p (Z-1)/p dp , where Z = pV/nRT = compressibility factor Ideal behavior For ideal behavior fJ = pJ (that is, J = 1). For this case J = J + RT ln (pJ/p) = J + RT ln pJ (division by p implied) Solvent (For liquid solutions. A is usually used to indicate the solvent. Vapor phase is assumed to behave ideally.) General expression A = A* + RT ln aA , where aA = pA/pA*. In this expression pA is the partial pressure of A above the solution and pA* is the vapor pressure of pure A. Reference state A*, the chemical potential of the pure liquid. This is a real reference state. Activity aA, the "effective mole fraction" of the solvent. aA = pA/pA* Activity coefficient A, defined by the expression aA = AXA, where XA is the mole fraction of A in the solution. Ideal behavior For ideal behavior aA = XA (that is, A = 1). For this case A = A* + RT ln XA Ideal behavior corresponds to the solvent obeying Raoult's law pA = XA pA* Solute, mole fraction (For liquid solutions. B is usually used to indicate the solute.) General expression B = B+ + RT ln aB , where aB = pB/KB, KB is the Henry's law constant. Reference state B+ = B* + RT ln (KB/pB*) , the chemical potential of pure B under conditions where only A-B interactions occur. This represents a hypothetical reference state for B. Activity aB, the "effective mole fraction" of the solute. aB = pB/KB. Activity coefficient B, defined by the expression aB = B XB, where XB is the mole fraction of B in the solution. Ideal behavior For ideal behavior aB = XB (that is, B = 1). For this case B= B+ + RT ln XB Ideal behavior corresponds to the solute obeying Henry's law pB = KBXB Solute, molality (For liquid solutions. Note: I have used bB for molality, the symbol used by Atkins, though many books use mB for the solute molality. Also note that for dilute aqueous solutions molality and molarity are approximately equal, in which case molarity is often used for solute concentration) General expression B = B + RT ln aB Reference state B= B+ + RT ln , where is the conversion factor between mole fraction and molality in the dilute solution limit XB = bB/bB , where bB is solute molality. bB is the reference molality of 1 mole/kg and ideal solute behavior. This therefore represents a hypothetical reference state for B. Activity aB, the "effective molality" of the solute, aB = pB/KB’, where KB is the constant from Henry's law, which in terms of molality is pB = (bB/bB) KB , KB = KB Activity coefficient B, defined by the expression aB = B bB/bB Ideal behavior For ideal behavior aB = bB/bB (that is, B = 1). For this case B= B + RT ln(bB/bB). Ideal behavior corresponds to the solute obeying Henry's law, in terms of molality.