Question 10.2.1: Using Azeotropic Data to Predict VLE of a Binary Mixture Ben...

Using Azeotropic Data to Predict VLE of a Binary Mixture Benzene and cyclohexane form an azeotrope at 0.525 mole fraction benzene at a temperature of 77.6°C and a total pressure of 1.013 bar. At this temperature the vapor pressure of pure benzene is 0.993 bar, and that of pure cyclohexane is 0.980 bar.

a. Using the van Laar model, estimate the activity coefficients of benzene and cyclohexane over the whole composition range. Use this activity coefficient information to compute the equilibrium pressure versus liquid composition diagram and the equilibrium vapor composition versus liquid composition diagram at 77.6°C.

b. Make predictions for the activity coefficients of benzene and cyclohexane using regular solution theory, and compare these with the results obtained in part (a).

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a. The van Laar model. The starting point is the equilibrium relation

 

\bar{f}_{ i }^{ L }(T, P, \underline{x})=\bar{f}_{ i }^{ V }(T, P, \underline{y})

 

which, at the pressures here, reduces to

 

x_{ i } \gamma_{ i } P_{ i }^{ vap }=y_{ i } P

 

Since x_{ i }=y_{ i } at an azeotropic point, we have \gamma_{ i }=P / P_{ i }^{\text {vap }} \text {, so that at } x_{ B }=0.525

 

\gamma_{ B }\left(x_{ B }=0.525\right)=\frac{1.013}{0.993}=1.020

 

\gamma_{ C }\left(x_{ B }=0.525\right)=\frac{1.013}{0.980}=1.034

 

Using Eqs. 9.5-10, we obtain \alpha=0.125 \text { and } \beta=0.0919. Therefore,

 

\begin{aligned}\alpha &=\left(1+\frac{x_{2} \ln \gamma_{2}}{x_{1} \ln \gamma_{1}}\right)^{2} \ln \gamma_{1} \\\beta &=\left(1+\frac{x_{1} \ln \gamma_{1}}{x_{2} \ln \gamma_{2}}\right)^{2} \ln \gamma_{2}\end{aligned} (9.5-10)

 

\ln \gamma_{ B }=\frac{0.125}{\left[1+1.360\left(\frac{x_{ B }}{x_{ C }}\right)\right]^{2}} \quad \text { and } \quad \ln \gamma_{ C }=\frac{0.0919}{\left[1+0.736\left(\frac{x_{ C }}{x_{ B }}\right)\right]^{2}} (i)

 

The values of the activity coefficients for benzene (B) and cyclohexane (C) calculated from these equations are given in the following table and Fig. 1.

To compute the composition of the vapor in equilibrium with the liquid we use Eqs. 10.1-1b

 

x_{ i } \gamma_{ i }(T, P, \underline{x}) P_{ i }^{ vap }(T)=y_{ i } P (10.1-1b)

 

x_{ B } \gamma_{ B } P_{ B }^{ vap }=y_{ B } P \quad \text { and } \quad x_{ C } \gamma_{ C } P_{ C }^{ vap }=y_{ C } P (ii)

 

and Eq. 10.1-2b

 

\sum x_{ i } \gamma_{ i }(T, P, \underline{x}) P_{ i }^{ vap }(T)=P (10.1-2b)

 

x_{ B } \gamma_{ B } P_{ B }^{\text {vap }}+x_{ C } \gamma_{ C } P_{ C }^{ vap }=P (iii)

 

van Laar Regular Solution
x_{ B } \gamma_{ B } \gamma_{ C } y_{ B } P (bar) \gamma_{ B } \gamma_{ C }
0 1.13 1.00 0 0.980 1.14 1.00
0.1 1.10 1.00 0.110 0.992 1.11 1.00
0.2 1.07 1.01 0.212 1.001 1.09 1.00
0.3 1.05 1.01 0.311 1.006 1.07 1.01
0.4 1.03 1.02 0.406 1.012 1.06 1.02
0.5 1.02 1.03 0.501 1.013 1.04 1.03
0.525 1.02 1.03 0.525 1.013 1.04 1.04
0.6 1.01 1.04 0.596 1.010 1.03 1.05
0.7 1.01 1.05 0.693 1.006 1.02 1.07
0.8 1.00 1.07 0.792 1.005 1.01 1.10
0.9 1.00 1.08 0.894 1.000 1.00 1.13
1.0 1.00 1.10 1.0 0.993 1.00 1.17

 

In these equations the vapor compositions, y_{ B } \text { and } y_{ C }, and the equilibrium pressure P are unknown (the equilibrium pressure is 1.013 bar only at x_{ B }=0.525). The solution is obtained by choosing a value of x_{ B }, \operatorname{using} x_{ C }=1-x_{ B }, and computing \gamma_{ B } \text { and } \gamma_{ C } from Eqs. i, and the total pressure from Eq. iii. The vapor-phase mole fractions are then computed from Eqs. ii. The results of this calculation are given in the table and Fig. 2.

b. Regular solution model. Since benzene and cyclohexane are nonpolar, and their solubility parameters are given in Table 9.6-1, the activity coefficients can be predicted using Eqs. 9.6-10. The results of this calculation are given in the table. The agreement between the correlation of the data using the van Laar model and the predictions (without reference to the experimental data) using the regular solution is good in this case.

 

\begin{array}{l}R T \ln \gamma_{1}=\underline{V}_{1} \Phi_{2}^{2}\left[\delta_{1}-\delta_{2}\right]^{2} \\R T \ln \gamma_{2}=\underline{V}_{2} \Phi_{1}^{2}\left[\delta_{1}-\delta_{2}\right]^{2}\end{array} (9.6-10)

 

Note

From Fig. 2 we see that for this mixture the compositions of the vapor and liquid in equilibrium are very close. An important implication of this is that it will be very difficult to separate benzene and cyclohexane from their mixture using distillation.

 

Table 9.6-1 Molar Liquid Volumes and Solubility Parameters of Some Nonpolar Liquids
\underline{V}^{ L }( cc / mol ) \delta( cal / cc )^{1 / 2}
Liquefied gases at 90 K
Nitrogen 38.1 5.3
Carbon monoxide 37.1 5.7
Argon 29 6.8
Oxygen 28 7.2
Methane 35.3 7.4
Carbon tetrafluoride 46 8.3
Ethane 45.7 9.5
Liquid solvents at 25°C
Perfluoro-n-heptane 226 6
Neopentane 122 6.2
Isopentane 117 6.8
n-Pentane 116 7.1
n-Hexane 132 7.3
1-Hexene 126 7.3
n-Octane 164 7.5
n-Hexadecane 294 8
Cyclohexane 109 8.2
Carbon tetrachloride 97 8.6
Ethyl benzene 123 8.8
Toluene 107 8.9
Benzene 89 9.2
Styrene 116 9.3
Tetrachloroethylene 103 9.3
Carbon disulfide 61 10
Bromine 51 11.5
Source: J. M. Prausnitz, Molecular Thermodynamics of Fluid-Phase Equilibria. 1969. Reprinted with permission from Prentice-Hall, Englewood Cliffs, N.J.
Note: In regular solution theory the solubility parameter has traditionally been given in the units shown. For this reason the traditional units, rather than SI units, appear in this table.
10.2.1
10.2.1.

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