Question 6.12: A phase diagram is drawn for a mixture of two substances at ...

A phase diagram is drawn for a mixture of two substances at a fixed pressure p with a liquid phase and a gaseous phase (Fig. 6.5). The substances are labelled 1 and 2 and the diagram is shown as a function of the concentration c_1 of substance 1. There is a range of temperature for which there is coexistence of two phases. Answer the following questions, treating the concentrations c^A_1 and  c^B_1 as given values.
a) Apply the Gibbs phase rule (6.62) to find the number of degrees of freedom when two phases coexist at a fixed pressure p.

f = 2 + m(r − 1) − r (m − 1) = r − m + 2
b) We distill a substance 1 with an initial concentration c^A_1 by heating the liquid up to the temperature T_C. Determine the final concentration of substance 1 after distillation.
c) A mixture with a concentration c^C_1 of substance 1 is put in a container. The mixture is brought to a temperature T_C while the pressure remains at p. Establish that,

N_\ell (c^C_1 - c^A_1) = N _g (c^B_1 - c^C_1) .

where N_\ell the amount of mixture in the liquid phase, and N_g that in the gas phase. This is known as the lever rule.

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a) According to Gibbs phase rule (6.62) r = 2 and m = 2 imply that f = 2. If the pressure p is fixed then there is only one degree of freedom. If we choose c_1 as the variable, then the temperature where the two phases coexist can be read on the phase diagram for each value of c_1.

f = 2 + m(r − 1) − r (m − 1) = r − m + 2

b) When the liquid mixture reaches the temperature T_C, a vaporisation takes place. After condensation, the concentration of substance 1 is c^B_1.

c) The concentration c^A_1 , c^B_1 and c^C_1 are defined as,

c^A_1 = \frac {N_{\ell 1}}{N_{\ell }}      and    c^B_1 = \frac {N_{g 1}}{N_{g }}      and    c^C_1 = \frac{N_{\ell 1 }+ N_{g1}}{N_{\ell }+ N_{g}} .

where N_{\ell} = N_{\ell 1} + N_{\ell 2} and N_g = N_{g1} + N_{g2} are the amounts of substances 1 and 2 in the liquid phase \ell and the gaseous phase g. Thus,

(N_\ell + N_g) c^C_1 =  N_\ell  c^A_1 + N_g c^B_1.

which implies that

N_\ell ( c^C_1 – c^A_1 ) = N_g ( c^B_1 – c^C_1) .

This result would be obtained if we had two ‘weights’ N_\ell and N_g hanging from the ends of a mechanical lever of length AB at equilibrium around its axis at C.

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