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               Chapter 10                Since x   x   1, we have dx   dx   0, and the last equation becomes
                                                                          B
                                                    B
                                               A
                                                                    A
               Nonideal Solutions
                                                           d ln g   1x >x 2 d ln g    const. T, P          (10.22)
                                                                B      A  B      A
                                         Integrating between states 1 and 2, and choosing Convention II, we get
                                                   ln g II,B,2    ln g II,B,1       2      x A     d  ln g II,A    const. T, P  (10.23)
                                                                         1  1   x A
                                         Let state 1 be pure solvent A. Then g    1 [Eq. (10.10)] and ln g    0. We plot
                                                                        II,B,1                    II,B,1
                                         x /(1   x ) versus ln g  . The area under the curve from x   1 to x   x  gives
                                          A      A           II,A                           A        A    A,2
                                          ln g    . Even though the integrand x /(1   x ) → q as x → 1, the area under the
                                              II,B,2                      A      A          A
                                         curve is finite; but the infinity makes it hard to accurately evaluate the integral in
                                         (10.23) graphically. A convenient way to avoid this infinity is discussed in Prob. 10.34.
                                         [Equation (10.23) is for a two-component solution. Surprisingly, if activity-coefficient
                                         data for one component of a multicomponent solution are available over the full range
                                         of compositions, one can find the activity coefficients of all the other components; see
                                         Pitzer (1995) pp. 220, 250, 300.]
                                             Some activity coefficients for aqueous solutions of sucrose at 25°C calculated
                                         from vapor-pressure measurements and the Gibbs–Duhem equation are:
                                         x(H O)           0.999     0.995    0.980    0.960     0.930     0.900
                                            2
                                         g (H O)          1.0000    0.9999   0.998    0.990     0.968     0.939
                                          II  2
                                         g (C H O )       1.009     1.047    1.231    1.58      2.31      3.23
                                          II  12  22  11
                                             Note from (10.22) that g  must increase when g   decreases at constant T
                                                                 II,sucrose               II,H 2 O
                                         and P. Because of the large size of a sucrose molecule (molecular weight 342) com-
                                         pared with a water molecule, the mole-fraction values can mislead one into thinking
                                         that a solution is more dilute than it actually is. For example, in an aqueous sucrose
                                         solution with x(sucrose)   0.10, 62% of the atoms are in sucrose molecules, and the
                                         solution is extremely concentrated. Even though only 1 molecule in 10 is sucrose, the
                                         large size of sucrose molecules makes it highly likely for a given sucrose molecule to
                                         be close to several other sucrose molecules, and g  deviates greatly from 1.
                                                                                   II,sucrose
                                             Aqueous sucrose solutions have g    1 and g    1. The same reasoning used
                                                                         II,i        II,A
                                         for acetone–chloroform solutions shows that sucrose–H O interactions are more fa-
                                                                                         2
                                         vorable than sucrose–sucrose interactions.
                                         Other Methods for Finding Activity Coefficients
                                         Some other phase-equilibrium properties that can be used to find activity coefficients
                                         are freezing points of solutions (Sec. 12.3) and osmotic pressures of solutions
                                         (Sec. 12.4). Activity coefficients of electrolytes in solution can be found from galvanic-
                                         cell data (Sec. 13.9).
                                             In industrial processes, liquid mixtures are often separated into their pure compo-
                                         nents by distillation. The efficient design of distillation apparatus requires knowledge
                                         of the partial vapor pressures of the mixture’s components, which in turn requires
                                         knowledge of the activity coefficients in the mixture. Therefore, chemical engineers
                                         have devised various methods of estimating activity coefficients. Group-contribution
                                         methods express the activity coefficients as functions of the mole fractions and of pa-
                                         rameters for interactions between the various chemical groups in the molecules of the
                                         components of the solution. The parameter values were chosen to give good fits to
                                         known activity coefficients. Such group-contribution methods (with names like ASOG
                                         and UNIFAC) often work fairly well but sometimes give very inaccurate results.
                                             Other approaches to estimating activity coefficients are considered in Probs. 10.13
                                         to 10.19. A thorough discussion of activity-coefficient estimation methods in liquid
                                         mixtures is given in Poling, Prausnitz, and O’Connell, chap. 8.
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