By our equilibrium constraint,
By our ideal solution approximation in both phases, the equilibrium criteria becomes
Now we need to substitute the expressions for fiV and fiL that we developed in Chapter 9. The fugacity of the pure vapor comes from Eqn. 9.25:
The fugacity of the liquid comes from Eqn. 9.39:
Combining Eqns. 10.70–10.72,
Writing in terms of the Ki ratio,
Note: at reasonably low pressures,
resulting in Raoult’s Law,
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