“Phase Equilibriain Materials” · 2018. 1. 30. · -Binary phase diagrams 1) Simple Phase...
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1 Advanced Physical Metallurgy Advanced Physical Metallurgy “ “ Phase Phase Equilibria Equilibria in Materials in Materials ” ” Eun Eun Soo Soo Park Park Office: 33-316 Telephone: 880-7221 Email: [email protected] Office hours: by an appointment 2009 fall 10. 01. 2009
Transcript of “Phase Equilibriain Materials” · 2018. 1. 30. · -Binary phase diagrams 1) Simple Phase...
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Advanced Physical MetallurgyAdvanced Physical Metallurgy
““Phase Phase EquilibriaEquilibria in Materialsin Materials””
EunEun SooSoo ParkPark
Office: 33-316 Telephone: 880-7221Email: [email protected] hours: by an appointment
2009 fall
10. 01. 2009
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Contents for previous class- Equilibrium in Heterogeneous Systems
- Binary phase diagrams1) Simple Phase Diagrams
3) Simple Eutectic Systems
G0β > G0
α > G0α+β α + β separation unified chemical potential
Assume: (1) completely miscible in solid and liquid.(2) Both are ideal soln.
0=Δ SmixH0=Δ L
mixH
2) Variant of the simple phase diagram0>Δ>Δ l
mixmix HH α 0<Δ<Δ lmixmix HH α
miscibility gab Ordered phase
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Contents for today’s class
- Gibbs Phase Rule
- Eutectoid reaction
- Peritectic reaction
Formation of intermediate phases by peritectic reaction
Non-stoichiometeric compounds
- Congruent transformations
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The Gibbs Phase Rule
In chemistry, Gibbs' phase rule describes the possible number of degrees of freedom (F) in a closed system at equilibrium, in terms of the number of separate phases (P) and the number of chemical components (C) in the system. It was deduced from thermodynamicprinciples by Josiah Willard Gibbs in the 1870s.
In general, Gibbs' rule then follows, as:
F = C − P + 2 (from T, P). From Wikipedia, the free encyclopedia
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For a binary system the equilibria possible are summarised below.
P=cP=c--11P=cP=cP=c+1P=c+1
Invariant reactions which have been observed in binary diagrams are listed below,together with the nomenclature given to such reactions.
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1 single phaseF = C - P + 1
= 2 - 1 + 1= 2
can vary T and composition independently
2 two phaseF = C - P + 1
= 2 - 2 + 1= 1
can vary T orcomposition
3 eutectic pointF = C - P + 1
= 2 - 3 + 1= 0
can’t vary T or composition
For Constant Pressure, P + F = C + 1
The Gibbs Phase Rule
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The Gibbs Phase Rule
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Eutectoid reaction
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Peritectic reaction
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Peritectic reaction0>Δ>Δ l
mixmix HH α
Considerable difference between the melting points
Eutectic reaction
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Eutectic: L→α+β Peritectic: L+α → β
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Peritectic reaction
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Peritectic reaction
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4.3.4. Formation of intermediate phases by peritectic reaction
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4.3.4. Formation of intermediate phases by peritectic reaction
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4.3.4. Formation of intermediate phases by peritectic reaction
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4.3.4. Formation of intermediate phases by peritectic reaction
(1)
(2)
(3)
(4)
(5)
(1)
(2)
(3)
(4)
(5)
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(2)
Peritectic point virtually coincides with the liquid composition.But, thermodynamically, points P and b is not possible to coincide.
0)( =−A
lS
dXdTSS
))(()(A
lA
A
SA
BAA
lS
dXdX
dXdX
dXdTSS −−=− μμ
lB
SB
lA
SA
ls dGdG μμμμ === ,,At equilibrium,
0/, =≠ AlS dXdTSS
At const P and differentiating with respect toXA
lA
SA XX =
Peritectic point and the liquid composition are so close to each other that the experimental techniquies used were not able to distinguish them.
Temp. maximum or minimum must be present.
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(1)
Decreasing solubility of Zn in Cu with rise in temperaturein contrast to the normal decrease in solubility with fall in temperature
Due to an equilibrium with a disordered intermediate phase(e.g. the β phase above 454 ℃, Fig. 71)
This has been explained as being due to a greater relative movement of the free energy curve of the intermediate phase compared with the αsolid solution with rise in temperature.
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4.3.5. Non-stoichiometeric compounds
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4.3.5. Non-stoichiometeric compounds
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θ phase in the Cu-Al system is usually denoted as CuAl2 although the composition XCu=1/3, XAl=2/3 is not covered by the θ field on the phase diagram.
4.3.5. Non-stoichiometeric compounds
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4.4. Congruent transformations
Congruent transformation:a melting point minimum, a melting point maximum, and a criticaltemperature associated with a order-disorder transformation
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4.4. Congruent transformations
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4.4. Congruent transformations
Relationship between phase diagrams containing congruent and incongruent intermediate phases
