Ch08 Notes

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9/24/2015 1 Phase Diagrams (Ch. 8) Phase Diagram For Water Figure 8.1 After W. G. Moffatt, et al., “The Structure and Properties of Materials,” vol I: “Structure,” Wiley, 1965, p.151

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Notes for IUPUI ME 344

Transcript of Ch08 Notes

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Phase Diagrams (Ch. 8)

Phase Diagram For Water

Figure 8.1

After W. G. Moffatt, et al., “The Structure and Properties of Materials,” vol I: “Structure,” Wiley, 1965, p.151

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Gibbs Phase Rule

Cooling Curve for water

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Another Triple Point Example

Figure 8.2

After W. G. Moffatt, et al., “The Structure and Properties of Materials,” vol I: “Structure,” Wiley, 1965, p.151

Cooling curves for Alloys

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Binary Isomorphous Alloy Systems

• Example: Cu-Ni solution.

Figure 8.3

Adapted from “Metals Handbook,” vol. 8, 8th ed., American society of Metals, 1973, p. 294.

The Lever Rule

• The Lever rule gives the weight % of phases in any two phase regions.

Wt fraction of solid phase= Xs = w0 – w1

ws – w1

Wt fraction of liquid phase= X1 = ws – w0

ws – w1

Figure 8.5

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Example

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Equilibrium Solidification = Cored Structure

Non Equilibrium Still Cored

Figure 8.7

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How to fix this?

Binary Alloy Systems

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Binary Alloy

Binary Alloy

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Binary Alloy

Binary Alloy

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Binary Alloy

Binary Alloy

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Slow Cooling of 60% Pb – 40% Sn alloy

Figure 8.13

Figure 8.12

From J. Nutting and R. G. Baker, “Microstructure of Metals,” Institute of Metals, London, 1965,p.19.

Binary Peritectic Alloy System

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Peritectic Alloy System

Binary Monotectic Systems

Metals Handbook,” vol. 8: “Metallography Structures and Phase Diagrams,” 8th ed., American Society of Metals, 1973, p. 296.

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Systems

Eutectic

Eutectoid

Peritectic

Peritectoid

Monotectic

Metals Handbook,” vol. 8: “Metallography Structures and Phase Diagrams,” 8th ed., American Society of Metals, 1973, p. 296.

Intermediate Phases and Compounds

Figure 8.25“Metals Handbook,” vol. 8: “Metallography Structures and Phase Diagrams,” 8th ed., American Society of Metals, 1973, p. 301

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Aluminum Copper Binary Phase Diagram

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Impossibilities Diagram

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Impossibilities

A: The liquidus and solidus must meet at the melting point of the pure element. B: Two liquidus curves must meet at one composition at a eutectic temperature. C: A tie line must terminate at a phase boundary. D: Two solvus boundaries (or two liquidus, or two solidus, or a solidus and a solvus) of the same phase must intersect at one composition at an invariant temperature. E: A phase boundary must extrapolate into a two-phase field after crossing an invariant point. F: A two-phase field cannot be extended to a pure element end. G: Two boundaries of g must not be continuous at the invariant temperature. They must cross one another. H: An invariant temperature line should involve equilibrium among three phases.I: There should be a two-phase field between two single phase fields.

J: When two phase boundaries touch at a point, they should touch at an extremity of temperature. K: A touching liquidus and solidus (or any two touching boundaries) must have a horizontal common tangent at the congruent point. In this case, the slope of the solidus appears to be discontinuous at the melting point. L: A local minimum point in the lower part of a single-phase field cannot be drawn without an additional boundary in contact with it (minimum congruent point or monotectic reaction in this case). M: A local maximum point in the lower part of a single-phase field cannot be drawn without a monotectic, monotectoid, syntactic, and syntectoid reaction occurring at a lower temperature. Alternatively, a solidus curve must be drawn to touch the liquidus at point M. (If the maximum is not local, as in a miscibility gap, this is not a phase rule violation.)N: The temperature of an invariant reaction must be constant. (The reaction line must be horizontal.) O: A phase boundary cannot terminate within a phase field (except the case when the boundary is unknown beyond this point). P: The liquidus should not have a discontinuous sharp peak at the melting point of a compound. (See exceptions below.) Q: The compositions of all three phases at an invariant reaction must be different. R: Temperatures of liquidus and solidus (or any two boundaries) must either increase or decrease together from one point on the pure element line as the content of a second element increases. S: A four-phase equilibrium is not allowed in a binary system. (See exceptions below.) T: Two separate phase boundaries that create a two-phase field between two phases in equilibrium should not cross one another.

Intermediate Compounds

Figure 8.27

Metals Handbook,” vol. 8: American Society of Metals, 1973, p. 314.

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Ternary Phase Diagrams

Figure 8.28

Ternary Phase Diagrams

Figure 8.28

B

A

C

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Ternary Phase Diagram (Cont..)

• Example:- Iron-Chromium-Nickel phase diagrams.

Figure 8.30

After “Metals Handbook,” vol. 8: American Society of Metals, 1973, p. 425.