## PHASE RULE

Phase Rule as applied to Binary Diagrams

Binary diagrams are drawn for atmospheric pressures, thus P is no longer a variable and the Phase Rule becomes:

**P + F = C + 1** (Condensed Phase Rule)

With reference to the hypothetical binary diagram:

- At X

Point X lies within the liquid field,

- P = 1 - Liquid
- C = 2 - two components A and B
- F = 2 - two degrees of freedom, giving a divariant area.
- To maintain equilibrium, i.e. to keep the single phase Liquid stable, T and X may be varied independently.

- At Y

Point Y lies on the boundary curve between the fields of Liquid and A + Liq.
- P = 2 - Solid A and Liquid
- C = 2 - two components A and B,
- F = 1 - one degree of freedom yielding a univariant curve.
- To maintain equilibrium, i.e. to stay on the boundary curve, Fixing T automatically fixes X.

- At E

Point E is the eutectic, the point where the liquidus and solidus intersect.
- P = 3 - Solid A, Solid B and Liquid,
- C = 2 - two components A and B,
- F = 0 - no degrees of freedom, an invariant point.
- No degrees of freedom, all 3 phases coexist in equilibrium, changing either temperature or compostion from the point represented by E will cause one or more of the phases to disappear, thus changing the value for P in the phase rule equation.