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Equilibrium Compositions as Functions of Pressure and Temperature

At the low pressure P, both components can exist as liquids in their pure state, wiA and Tg representing their boiling point temperatures the T-x-y curves in this case cover the whole composition range. Moving to higher pressures we notice that, at 2, as the composition of A increases we reach the critical point C, where y = x/, and that at the still higher pressure P3, two critical points are present the T-x-y curves do not cover the whole composition range any more. [Pg.516]

The practical implications of this behavior in terms of separating a mixture of A and B are apparent at Pj, pure A and B can be recovered at P2, only B and at P3, neither. [Pg.516]

Similar phase diagrams are obtained if we consider the effect of temperature on Ae P-x-y relationship of a binary mixture. [Pg.516]


See other pages where Equilibrium Compositions as Functions of Pressure and Temperature is mentioned: [Pg.512]    [Pg.516]   


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A composition

As a function of temperature

Composite functionals

Composite temperature

Composition of functions

Composition temperature, pressure and

Compositional equilibrium

Compositions and temperatures

Equilibrium compositions

Equilibrium function

Equilibrium function of temperature

Equilibrium pressure

Equilibrium temperature

Function of temperature

Functional Pressure

Functional composites

Pressure equilibrium and

Pressure-composition-temperature

Temperature as a function

Temperature pressure and

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