Ch09- Phase Diagrams
Transcript of Ch09- Phase Diagrams
CHAPTER 9Phase Diagrams—
EquilibriumMicrostructural
Development
The microstructure of a slowly cooled “eutec-tic” soft solder (≈ 38 wt % Pb − wt % Sn)consists of a lamellar structure of tin-rich solidsolution (white) and lead-rich solid solution(dark), 375X. (From ASM Handbook, Vol.3: Alloy Phase Diagrams, ASM International,Materials Park, Ohio, 1992.)
Figure 9-1 Single-phase microstructure of commerciallypure molybdenum, 200×. Although there are manygrains in this microstructure, each grain has the same,uniform composition. (From Metals Handbook, 8thed., Vol. 7: Atlas of Microstructures, American Societyfor Metals, Metals Park, Ohio, 1972.)
Figure 9-2 Two-phase microstructure of pearlite found ina steel with 0.8 wt % C, 500×. This carbon content isan average of the carbon content in each of the alter-nating layers of ferrite (with <0.02 wt % C) and ce-mentite (a compound, Fe3C, which contains 6.7 wt %C). The narrower layers are the cementite phase. (FromMetals Handbook, 9th ed., Vol. 9: Metallography andMicrostructures, American Society for Metals, MetalsPark, Ohio, 1985.)
TemperatureGas
Liquid
Solid
1 atmPressure (log scale)
(a) (b)
Water
Ice
Steam100
0
T(°C)
Figure 9-3 (a) Schematic representation of the one-component phase diagram for H2O.(b) A projection of the phase diagram information at 1 atm generates a temperaturescale labeled with the familiar transformation temperatures for H2O (melting at 0◦Cand boiling at 100◦C).
Temperature
Gas Liquid
1 atmPressure (log scale)
(a) (b)
Liquid
T(˚C)
15381394
910
Figure 9-4 (a) Schematic representation of the one-component phase diagram for pureiron. (b) A projection of the phase diagram information at 1 atm generates a tempera-ture scale labeled with important transformation temperatures for iron. This projectionwill become one end of important binary diagrams such as Figure 9–19.
Tem
pera
ture
Melting pointof A
Melting pointof B
A B0 20 40 60 80 100 ← wt % B
100 80 60 40 20 0 ←wt % A
Composition (wt %)
L + SS
Liquidus
Solidus
SS
L
Figure 9-5 Binary phase diagram showing complete solid solution. The liquid-phase field is labeled L and the solid solution is designated SS. Note thetwo-phase region labeled L + SS.
A B
Compositionof SS at T1
Compositionof L at T1
Statepoint
Systemcomposition
L + SS
Systemtemperature
X1
SS
L
T1
Figure 9-6 The compositions of the phases in a two-phase region of the phasediagram are determined by a tie line (the horizontal line connecting the phasecompositions at the system temperature).
Composition
Temperature
A B
F = C – P + 1
F = 2 – 1 + 1 = 2 F = 1 – 2 + 1 = 0
F = 2 – 1 + 1 = 2
F = 2 – 2 + 1 = 1
Figure 9-7 Application of Gibbs phase rule (Equation 9.2) to various pointsin the phase diagram of Figure 9–5.
A B
Systemcomposition
Temperature
T1L1
Lsystem
Composition
SS1
SSsystem
All liquid (Lsystem)
Crystallites of SS1in matrix of L1
Polycrystalline solid(SSsystem)
Figure 9-8 Various microstructures characteristic of different regions inthe complete solid-solution phase diagram.
Cu 20 4010
10
1084.87˚
˚C
1455˚1500
1400
1300
1200
1100
1000
900
800
700
600
500
20 30 40 50 60 70 80 90
30 50Weight percentage nickel
Atomic percentage nickel
70 9060 80 Ni
L
Figure 9-9 Cu–Ni phase diagram. (After Metals Handbook, 8th ed., Vol. 8:Metallography, Structures, and Phase Diagrams, American Society forMetals, Metals Park, Ohio, 1973, and Binary Alloy Phase Diagrams, Vol.1, T. B. Massalski, ed., American Society for Metals, Metals Park, Ohio,1986.)
2800
2600
2400
2200
2000
˚C
NiO 20 40 60
L + SS
SS
L
80 MgO
Mole % MgO
Figure 9-10 NiO–MgO phase diagram. (After PhaseDiagrams for Ceramists, Vol. 1, American CeramicSociety, Columbus, Ohio, 1964.)
A
L
A + LL + B
A + B
B
Eutectictemperature
EutecticComposition
Tem
pera
ture
Composition
Liquidus
Solidus
Figure 9-11 Binary eutectic phase diagram showing no solid so-lution. This general appearance can be contrasted to the op-posite case of complete solid solution illustrated in Figure 9–5.
A BComposition
Leutectic
Temperature
Crystallites of Ain matrix of L1
All liquid (Leutectic)
Crystallites of Bin matrix of L2
Eutectic microstructure—fine, alternating layers ofA and B
L1 L2
Figure 9-12 Various microstructures characteristic of different regions in a binary eutectic phase di-agram with no solid solution.
300
400
500
600
1.6 12.6577˚
1414˚
˚C
700660.452˚
800
900
1000
1100
1200
1300
1400
1500
A1 10 20 30 40 50 60 70 80 90
10 20 30 40 50 60 70 80 90
Si
Weight percentage, silicon
Atomic percentage, silicon
L
Figure 9-13 Al–Si phase diagram. (After Binary Alloy Phase Diagrams, Vol.1, T. B. Massalski, ed., American Society for Metals, Metals Park, Ohio,1986.)
L
A B
Tem
pera
ture
Composition
Figure 9-14 Binary eutectic phase diagram withlimited solid solution. The only differencefrom Figure 9–11 is the presence of solid-solutionregions α and β .
Leutectic
A B
Temperature
Composition
All liquid (Leutectic)
L1 L2
Figure 9-15 Various microstructures characteristic of different regions in the binary eutectic phase di-agram with limited solid solution. This illustration is essentially equivalent to Figure 9–12 exceptthat the solid phases are now solid solutions (α and β) rather than pure components (A and B).
10400˚C
327.502˚
300
200
100
0Pb 10 20 30 40
L
50 60 70 80 90 Sn
20 30 40 50 60
Atomic percentage tin
Weight percentage tin
70 80 90
19 183˚ 61.9 97.5
231.9681̊
13˚
Figure 9-16 Pb–Sn phase diagram. (After Metals Handbook, 8th ed., Vol. 8: Metallogra-phy, Structures, and Phase Diagrams, American Society for Metals, Metals Park, Ohio,1973, and Binary Alloy Phase Diagrams, Vol. 2, T. B. Massalski, ed., American Societyfor Metals, Metals Park, Ohio, 1986.)
L
A B
Temperature
Eutectoidtemperature
Eutectictemperature
Eutectoidcomposition
Eutecticcomposition
Composition
Figure 9-17 This eutectoid phase diagram contains both a eutectic reaction (Equa-tion 9.3) and its solid-state analog, a eutectoid reaction (Equation 9.4).
A B
Temperature
Composition
Figure 9-18 Representative microstructures for the eutectoid diagram of Figure 9–17.
Atomic percentage carbon˚C 2 5
L
10 15 20 251700
1538˚1495˚
1394˚
1148˚
2.11 4.30
L + Fe3C
Fe
Weight percentage carbon
1 2 3 4 5 6 7
727˚
0.02 0.77
6.69
1227˚C
912˚
1600
1500
1400
1300
1200
1100
1000
900
800
700
600
500
400
300
200
100
0
Fe3C(cementite)
Figure 9-19 Fe–Fe3C phase diagram. Note that the composi-tion axis is given in weight percent carbon even though Fe3C,and not carbon, is a component. (After Metals Handbook,8th ed., Vol. 8: Metallography, Structures, and Phase Di-agrams, American Society for Metals, Metals Park, Ohio,1973, and Binary Alloy Phase Diagrams, Vol. 1, T. B. Mas-salski, ed., American Society for Metals, Metals Park, Ohio,1986.)
Atomic percentage carbon
1538˚1495˚
1394˚
1154˚
4.26
L + C
Weight percentage carbon
738˚
2.08
0.02 0.68
912˚
C(graphite)
2˚C2200
2100
2000
1900
1800
1700
1600
1500
1400
1300
1200
1100
1000
900
800
700
600
500
400
300
200
100
0Fe 1 2 3 4 5 6 99 100
5 10 15 20 25
Figure 9-20 Fe–C phase diagram. The left side of this dia-gram is nearly identical to that for the Fe–Fe3C diagram(Figure 9–19). In this case, however, the intermediate com-pound Fe3C does not exist. (After Metals Handbook, 8thed., Vol. 8: Metallography, Structures, and Phase Dia-grams, American Society for Metals, Metals Park, Ohio,1973, and Binary Alloy Phase Diagrams, Vol. 1, T. B.Massalski, ed., American Society for Metals, Metals Park,Ohio, 1986.)
A AB
A + AB
AB + B
L + B
L + ABA + L
L
B
Temperature
Composition ofliquid formed upon
melting of AB
Composition
Figure 9-21 Peritectic phase diagram showing a peritec-tic reaction (Equation 9.5). For simplicity, no solidsolution is shown.
A AB
Crystallites of Bin matrix of L1
Polycrystalline solid(compound AB)
L
B
Temperature
Composition
Figure 9-22 Representative microstructures for the peritectic diagram ofFigure 9–21.
2200
2100L
2000
1900
1726˚
1587
1890˚
2054˚
1800
1700
1600
1500
140010 20 30 40 50 60 70 80 90 Al2O3
Mole % Al2O3
˚C
SiO2 (cristobalite) + L
SiO2 (cristobalite) + mullite(SS)
SiO2
mul
lite(
SS)
Al2O3 + mullite(SS)
L + Al2O3
L + mullite(SS)
Figure 9-23 Al2O3–SiO2 phase diagram. Mullite is an intermediate com-pound with ideal stoichiometry 3Al2O3 · 2SiO2. (After F. J. Klug, S.Prochazka, and R. H. Doremus, J. Am. Ceram. Soc. 70, 750 (1987).)
Figure 9-24 (a) Binary phase dia-gram with a congruently meltingintermediate compound, AB. Thisdiagram is equivalent to two sim-ple binary eutectic diagrams (theA–AB and AB–B systems). (b)For analysis of microstructure foran overall composition in the AB–B system, only that binary eutecticdiagram need be considered.
Tem
pera
ture
A
A + L
A + ABAB + B
L + ABAB + L B + L
AB
L
B
Composition
(a)
Tem
pera
ture
A
AB + B
AB + L B + L
AB
L
B
Composition
(b)
L + ABA + L
A + AB
Temperature
Composition(a)
A A2B AB AB2 AB4 B
L
Temperature
Composition
A A2B AB AB2 AB4 B
L
10 30 5020 40 60 8070 90MgO Al2O3
Spinal (SS) + Al2O3
L + Al2O3
Mole % Al2O3
3000
2500
Periclase (SS)+ L
Periclase (SS)
Periclase (SS) + spinel (SS)
L + spinel (SS)
L
2000
1500
1000
˚C
Spinel (SS)
Figure 9-26 MgO–Al2O3 phase diagram. Spinel is an intermediate com-pound with ideal stoichiometry MgO · Al2O3. (After Phase Diagramsfor Ceramists, Vol. 1, American Ceramic Society, Columbus, Ohio,1964.)
Atomic percentage, copper
Weight percentage, copper
300
400
500
600
700
800
900
1000
1100
Al 10
0 10 20 30 40 50 60 70 80 90 100
20 30 40 50 60 70 80 90 Cu
L
660.452˚
5.65 32.7548.2˚
53.5
52.5567˚
1084.87˚
˚C
η1
Figure 9-27 Al–Cu phase diagram. (After Binary Alloy Phase Diagrams, Vol. 1, T. B. Massalski,ed., American Society for Metals, Metals Park, Ohio, 1986.)
Atomic percentage, magnesium
Weight percentage, magnesium
100
200
300
400
500
600
700
Al 10
10
660.452˚ 650˚
87.436.1
17.1
450˚35.6
59.8437˚
66.7
20 30 40 50 60 70 80 90 100
20 30 40 50 60 70 80 90
˚C
L
δ
455˚
Mg
Figure 9-28 Al–Mg phase diagram. (After Binary Alloy Phase Diagrams, Vol. 1, T. B.Massalski, ed., American Society for Metals, Metals Park, Ohio, 1986.)
4501 2 3
400
350
300
250
200
150
1001
Cu
130010 20 30 40 50 60 70 80 90
1250
1200
1150
1100 1084.87º
37.5
59.8
80.5
56.5
69.8
36.832.5
39.0
ºC
L
1050
1000
950
900
850
800
750
700
650
600
550
500
450
400
350
300
250
200
150
100
50
010 205 15 25 35 45 55 65 75 85 9530 40 50
Weight percentage, zinc
Atomic percentage, zinc
60 70 80 90 Zn
Weight percentage Cu
Atomic percentage Cu
Zn 2 3
2.7
L 1.7 424
903º
835º
73.0
74.1
87.5
98.3
78.6 598º
456º468º48.9
45.5
99.7%at 100º
419.58º
424º97.3
700º
558º
Figure 9-29 Cu–Zn phase diagram. (After Metals Hand-book, 8th ed., Vol. 8: Metallography, Structures, andPhase Diagrams, American Society for Metals, MetalsPark, Ohio, 1973, and Binary Alloy Phase Diagrams,Vol. 1, T. B. Massalski, ed., American Society for Met-als, Metals Park, Ohio, 1986.)
CubicZrO2SS + ZrCaO3
Cub
ic Z
rO2S
S
Tetr
agon
al Z
rO2S
S
Tetr
agon
al Z
rO2S
S +
Cub
ic Z
rO2S
S
Mon
oclin
ic Z
rO2S
S +
Cub
ic Z
rO2S
S
4
2500
2000
1500
1000
500
0
8 12CaO (wt %)
16 20 24 28˚C
ZrO2 10 20 30 40 50CaO (mol %)
Figure 9-30 CaO–ZrO2 phase diagram. The dashed linesrepresent tentative results. (After Phase Diagrams forCeramists, Vol. 1, American Ceramic Society, Colum-bus, Ohio, 1964.)
Tem
pera
ture
Composition
A A2B AB AB2 AB4 B
L
Temperature
A
0 30 50 80 100
L
T1
L + SS
SS
BComposition (wt % B)mL + mSS = mtotal0.30mL + 0.80mSS = 0.50mtotal
→mL = 0.60mtotalmSS = 0.40mtotal
Figure 9-31 A more quantitative treatment of the tie lineintroduced in Figure 9–6 allows the amount of eachphase (L and SS) to be calculated by means of a massbalance (Equations 9.6 and 9.7).
(a)
(b)Fulcrum
Figure 9-32 The lever rule is a mechanical anal-ogy to the mass balance calculation. The(a) tie line in the two-phase region is analo-gous to (b) a lever balanced on a fulcrum.
Temperature
A
T1
T2
T3
SSsystem
SS3
SS2
SS1
Lsystem
L3
L2
L1
BComposition
100% liquid(Lsystem)
10% SS1 inmatrix of L1
40% SS2 inmatrix of L2
90% SS3 inmatrix of L3
100% Solid(SSsystem)
Figure 9-33 Microstructural development during the slow cooling of a50% A–50% B composition in a phase diagram with complete solidsolution. At each temperature, the amounts of the phases in the mi-crostructure correspond to a lever rule calculation. The microstruc-ture at T2 corresponds to the calculation in Figure 9–31.
100% liquid(Leutectic)
Leutectic
Temperature
T1
T2
CompositionA B
*The only differences from the T1 microstructure arethe phase compositions and the relative amounts ofeach phase. For example, the amount of b will beproportional to
Figure 9-34 Microstructural development during the slow coolingof a eutectic composition.
100% liquid(Lsystem = 80% B)
Temperature
T2 (= Teutectic + 1 )T3 (= Teutectic – 1 )
0 30 60 9080Composition (wt % B)A
100B
Lsystem
L2 L1
Figure 9-35 Microstructural development during the slow cooling of a hypereutectic com-position.
100% liquid(Lsystem = 40% B)
Temperature
T2 (= Teutectic + 1 )T3 (= Teutectic – 1 )
0 30 60 9040Composition (wt % B)A
100B
Lsystem
L1
Figure 9-36 Microstructural development during the slow cooling of a hypoeutectic com-position.
100% liquid(Lsystem = 10% B)
100% liquid(Lsystem = 20% B)uid
(Lsystem = 20%
Temperature
0 10
(a)
Composition (wt % B)A
100
B
Lsystem
L1
Temperature
0 10 20
(b)
Composition (wt % B)A
100
B
Lsystem
L1
Figure 9 37 Mi t t l d l t f t iti th t id th
Temperature
100% liquid(3% C)
0 3.0
Weight percentage carbon
6.7
L1
Figure 9-38 Microstructural development for white cast iron (of compo-sition 3.0 wt % C) shown with the aid of the Fe–Fe3C phase diagram.The resulting (low-temperature) sketch can be compared with a mi-crograph in Figure 11–1a.
Temperature
0 0.77 6.7Weight percentage carbon
Figure 9-39 Microstructural development for eutectoid steel (ofcomposition 0.77 wt % C). The resulting (low-temperature)sketch can be compared with the micrograph in Figure 9–2.
Temperature
Proeutectoid cementite+ pearlite
Weight percentage carbon
0 1.13 6.7
Figure 9-40 Microstructural development for a slowly cooled hypereutectoid steel(of composition 1.13 wt % C).
Temperature
Proeutectoid ferrite+ pearlite
0 0.50
Weight percentage carbon
6.7
Figure 9-41 Microstructural development for a slowly cooled hypoeutectoid steel(of composition 0.50 wt % C).
Temperature
0 3 100
Weight percentage carbon
C flakes (from eutecticand eutectoid reactions)in matrix of ferrite
L1
100% liquid(3% C)
Figure 9-42 Microstructural development for gray cast iron (of compo-sition 3.0 wt % C) shown on the Fe–C phase diagram. The resultinglow-temperature sketch can be compared with the micrograph inFigure 11–1b. A dramatic difference is that, in the actual microstruc-ture, a substantial amount of metastable pearlite was formed at theeutectoid temperature. It is also interesting to compare this sketchwith that for white cast iron in Figure 9–38. The small amount ofsilicon added to promote graphite precipitation is not shown in thistwo-component diagram.
T
The phase diagram for this alloy system is
A B