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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
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:
However,
is constant so we lose one degree of freedom:
In the two phase region--
--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:
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.
 |
Next: Classifying the Invariant Points:
Up: Lecture_30_web
Previous: Construction of Phase Diagrams
W. Craig Carter
2002-12-03