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Next: Classifying the Invariant Points: Up: Lecture_30_web Previous: Construction of Phase Diagrams

A Menagerie of Binary Phase Diagrams

The phase diagram in Figure 30-4 is the simplest possible two-component phase diagram at constant pressure.

Figure: The so-called "lens" phase diagram. The upper line is the limit of $ \ensuremath{{f}^{\mbox{solid}}} \rightarrow 1$ and is called called the solidus curve. The lower line is called the liquidus curve.
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Figure 30-6: A variation on the lens phase diagram.
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Consider how the Gibbs phase rule relates to the above phase diagrams.

The Gibbs phase rule is: \bgroup\color{blue}$ D= C + 2 -f$\egroup

However, \bgroup\color{blue}$ P$\egroup is constant so we lose one degree of freedom: \bgroup\color{blue}$ D = C +1 -f$\egroup

In the two phase region-- \bgroup\color{blue}$ D = 2 + 1 - 2 =1$\egroup--so there is one degree of freedom.

Question: What is the degree of freedom? What does it mean?


Consider another two-component phase diagram and see if it violates the Gibbs phase rule.

Figure 30-7: Is this a possible phase diagram?
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Consider the three-phase region: \bgroup\color{blue}$ D = C +1 - f = 0$\egroup

Because there are no degrees of freedom, the three-phase region must shrink to a point in a two component system. This places restrictions on the topology of binary phase diagrams.

The diagrams below illustrate how such an invariant point (i.e., three phase equilibria in a two component system) arises:

Figure 30-8: Liquid is stable at all compositions at this temperature.
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Figure 30-9: One of the solid phases becomes stable.
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Figure 30-10: The second solid phase becomes stable as well, but not at the same compositions as the first.
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Figure 30-11: At one unique temperature (the Eutectic) the two phase regions converge-this is the invariant point.
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Figure 30-12: Below the eutectic, the two solid phases are separated by a two-phase region.
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This yields the following phase diagram

Figure 30-13: The free curves from Figures 30-8 through 30-12, result in a eutectic phase diagram.
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next up previous
Next: Classifying the Invariant Points: Up: Lecture_30_web Previous: Construction of Phase Diagrams
W. Craig Carter 2002-12-03