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Devesh agrawal
Chapter 3: The Structure of Crystalline Solids 2
Chapter 3: The Structure of Crystalline Solids 3
A solid solution forms when, as the solute atoms are added to the host materials, the crystal structure is maintained, and no new structures are formed.
Chapter 3: The Structure of Crystalline Solids 4
Chapter 3: The Structure of Crystalline Solids 5
Chapter 3: The Structure of Crystalline Solids 6
Chapter 3: The Structure of Crystalline Solids 7
Hume-Rothery (1899-1968) was a metallurgist who studied the alloying of metals. His research was conducted at Oxford University where in 1958, he was appointed to the first chair in metallurgy.
His research led to some simple and useful rules on the extent to which an element might dissolve in a metal . The rules that he derived are paraphrased here. The rules are still used widely. For example, the miscibility gap in Au-Ni is correlated with the fact that the lattice parameter of Au is 1.15 times that of Ni, thus acting maximally according to Hume-Rothery .
Chapter 3: The Structure of Crystalline Solids 9
Chapter 3: The Structure of Crystalline Solids 10
Chapter 3: The Structure of Crystalline Solids 11
Chapter 3: The Structure of Crystalline Solids 12
Chapter 3: The Structure of Crystalline Solids 13
Chapter 3: The Structure of Crystalline Solids 14
Chapter 09: Phase Diagram 15
Introduction
Phase Diagrams are road maps
Chapter 09: Phase Diagram 16
Component: Pure metals/compounds of which an alloy is
composed
System: Alloy system, e.g., Iron-Carbon alloy system,
copper-nickel alloy system
Solid solutions
- Substitutional
- Interstitial
Chapter 09: Phase Diagram 17
Solubility Limit: Max concentration of solute atoms that
may dissolve in the solvent to form a solid solution.
-The solubility limit of sugar in water depends on the
temperature of water. At 20degree C, maximum solubility
of sugar in water is 65%.
Phases: Homogenous portion of a system that has uniform
physical and chemical properties.
-Every pure material is considered to be a phase, e.g.
solid, liquid and gas phase
Chapter 09: Phase Diagram 18
If more than one phase is present in a given system, each will have its own distinct properties and boundary separating the phases will exist across which there will be discontinuous and abrupt change in physical and chemical characteristicsSubstance can exist in two or more polymorphic forms (having FCC and BCC structure) each have separate phase and different properties. Sugar water example, sugar water syrup solution is one phase and solid sugar is another
Chapter 09: Phase Diagram 19
Source: William Callister 7th edition, chapter 09, page 254, figure 9.1
Chapter 09: Phase Diagram 20
Each phase has different phase physical properties
Microstructure
•Characterized by number of phases, proportions and the
manner of distribution of phases.
•Depends on: Alloying elements, concentrations, heat
treatment (temp, heating/cooling rate etc.)
Chapter 09: Phase Diagram 21
Free energy : It is function of the internal energy of a system
and also the randomness of atoms/molecules
Equilibrium : A system is at equlibrium,if its free energy is
at a minimum under some specified combination of Temp,
Pressure and Composition
Phase equilibrium : Phase is equilibrium if it is constant
with time in the phase characteristics of a systems. It refers,
when more than one phase are present in system.
Isomorphous: Complete solubility in both liquid and solid
states.
Chapter 09: Phase Diagram 22
Non-equilibrium state/Metastable: State of equilibrium
is never reached since the rate of approach to equilibrium
is very slow. This state may persist indefinitely,
experiencing only slight and almost imperceptible
changes as time progresses
Equilibrium phase diagram
•Represents the relationships between temperature and
compositions, and the quantities of phases in equilibrium
Chapter 3: The
Structure of Crystalline
Solids23
Gibbs Phase Rule
Chapter 3: The
Structure of Crystalline
Solids24
Chapter 3: The
Structure of Crystalline
Solids25
Unary Phase Diagram (Pressure-temperature diagram for Water)
The simplest phase diagrams are pressure-temperature diagrams of a single simple substance, such as water. The axes correspond to the pressure and temperature. The phase diagram shows, in pressure-temperature space, the lines of equilibrium or phase boundaries between the three phases of solid, liquid, and gas.
Chapter 3: The
Structure of Crystalline
Solids26
Chapter 3: The
Structure of Crystalline
Solids27
Chapter 3: The
Structure of Crystalline
Solids28
Chapter 09: Phase Diagram 29
Binary Isomorphous Systems
Source: William Callister 7th edition, chapter 09, page 259, figure 9.3 a&b
Chapter 09: Phase Diagram 30
Three kinds of infomation:
•What Phases are present at particular temp and comp.
•Determination of phase compositions( in term of
concentration of compoents) Using Tie Line or Isotherm.
To determine the composition (in wt% Ni and Cu) for
both the alpha and liquid phase for 35wt%Ni-65 wt%Cu at
1250 C. Composition of liquid phase is 32 wt% Ni and
composition of alpha phase is 43 wt%Ni.
•percentages/fractions of phases (Phase Amount) at
equilibrium.
Chapter 09: Phase Diagram 31
73%0.7332433543W
L
27%0.2732433235W
Where, WL: weight/mass fraction of liquid
At 1250°C and Co=35% Ni
Chapter 09: Phase Diagram 32
Lever Rule (Inverse lever rule)
1.Draw tie-line across the two phase region
2.Locate the overall composition (e.g., Co=35%Ni)
3.To compute the fraction of one phase, take the length of
the tie-line from the overall composition to the opposite
phase boundary and divide by the total tie line length
4.Repeat above procedure for the other phase.
Chapter 09: Phase Diagram 33
•When two phases are present,Sum of their mass fractions must be Equal to unity.---- (1)
•Mass of one of the component (CuOr Ni) that is present in both phasesMust be equal to the mass of that Component in the total alloy- (2)
Where, Cs and C both are same
Chapter 09: Phase Diagram 34
Lever Rule
Chapter 09: Phase Diagram 35
Development of microstructures
Chapter 09: Phase Diagram 36
Development of microstructures(Non Equilibrium Cooling)(
Chapter 09: Phase Diagram 37
Development of Microstructures
The compositions readjust with changes in temperature.
These changes occur through the process of diffusion.
Because diffusion is time-dependent, much more time is
required, at each temperature for compositional
adjustments. Diffusion rates decrease with temperature. In
reality, cooling rates are so fast that there is little time to
enable equilibrium cooling. Diffusion rate in liquid is
faster than solid
Chapter 09: Phase Diagram 38
•Because of fast cooling, there is a
non-uniform distribution of the two
elements for isomorphous alloys
“Segregation”
In the centre of each grain, the high
melting element solidifies first. At the
periphery, the low melting element
solidifies.
Non-Equilibrium Solidification
Chapter 09: Phase Diagram 39
Coring
Cored Structure: Concentration contours
•Undesirable less than optimal properties due to
inhomogeneity.
•Coring is eliminated by a homogenization Heat
treatment. At a temperature below the solidus point for the
composition; atomic diffusion causes homogenization.
Chapter 09: Phase Diagram 40
Mechanical Properties of Isomorphous Alloys
Source: William Callister 7th edition, chapter 09, page 268, figure 9.6
Chapter 09: Phase Diagram 41
•Solid solution hardening or an increase in strength and
hardness by the addition of the other component
•At an intermediate composition, the curve (TS Vs Comp)
passes through a maximum
Mechanical Properties of Isomorphous Alloys
Chapter 09: Phase Diagram 42
Binary eutectic systems
Chapter 09: Phase Diagram 43
Binary eutectic systems Continue …..
:Solid Solution of Ag in Cu-Rich solvent
:Solid solution of Cu in Ag-Rich solvent
Technically, : Pure Cu
: Pure Ag
Below BEG, only limited solid solubility takes place
Chapter 09: Phase Diagram 44
CEA: (solid) solubility limit for Ag in – phase (Cu-Rich)
HGF: Solubility limit for Cu in -phase (Ag-Rich)
CBA is between /(+) and /(+L) phase regions
•Max. at 7.9% Ag (780°C)
Binary eutectic systems Continue …..
•Decrease to zero at 1085°C (Melting point of pure Cu)
Chapter 09: Phase Diagram 45
For –phase CB: solvus line: /(+)
AB: Solidus line: /(+L)
General Rule: Single phase regions are always separated
from each other by a two phase region that consists of two
single phases that it separtes.
Binary eutectic systems Continue …..
Chapter 09: Phase Diagram 46
Prepare similar notes for -phase region
HGF is between
For -phase
HG: Solvus line and GF: Solidus line
Binary eutectic systems Continue …..
Chapter 09: Phase Diagram 47
Three two-phase regions: +L, +L and +
E: Eutectic invariant point
CE: 71.9 wt% Ag
Cu-Ag system: TE: 780°C
Binary eutectic systems Continue …..
Chapter 09: Phase Diagram 48
Binary Eutectic systems Continue …..
Eutectic Reaction:
Liquid Solid 1 + Solid 2
L +
L(CE) (C E) + (C E)
At E,
Chapter 09: Phase Diagram 49
Binary Eutectic systems Continue …..
For Cu-Ag system,
L(71.9 wt% Ag) (7.9 wt% Ag) + (91.2 wt% Ag)
Chapter 09: Phase Diagram 50
Binary Eutectic systems Continue …..
Solidus line at 780°C: Eutectic isotherm
Phase volume fractions represent proportions seen in the
microstructure; so they can be estimated from
microstructures, and the mechanical properties can be
estimated as well.
Chapter 09: Phase Diagram 51
Source: William Callister 7th edition, chapter 09, page 271, figure 9.8
Binary Eutectic systems Continue …..
Chapter 09: Phase Diagram 52
Chapter 09: Phase Diagram 53
Chapter 09: Phase Diagram 54
Chapter 09: Phase Diagram 55
Chapter 09: Phase Diagram 56
Chapter 09: Phase Diagram 57
Chapter 09: Phase Diagram 58
Chapter 09: Phase Diagram 59
Chapter 09: Phase Diagram 60
Chapter 09: Phase Diagram 61
62
Temperature Dependence of Transformation Rate
For the recrystallization of Cu, since
rate = 1/t0.5
rate increases with increasing temperature
• Rate often so slow that attainment of equilibrium state not possible!
Adapted from Fig. 11.11, Callister & Rethwisch 3e.(Fig. 11.11 adapted from B.F. Decker and D. Harker, "Recrystallization in Rolled Copper", Trans AIME, 188, 1950, p. 888.)
135C 119C 113C 102C 88C 43C
1 10 102 104
63
Transformations & Undercooling
• For transf. to occur, must cool to below 727°C (i.e., must “undercool”)
• Eutectoid transf. (Fe-Fe3C system): + Fe3C0.76 wt% C
0.022 wt% C6.7 wt% C
Fe 3
C (
cem
entit
e)
1600
1400
1200
1000
800
600
4000 1 2 3 4 5 6 6.7
L
(austenite)
+L
+Fe3C
+Fe3C
L+Fe3C
(Fe) C, wt%C
1148°C
T(°C)
ferrite
727°C
Eutectoid:Equil. Cooling: Ttransf. = 727ºC
T
Undercooling by Ttransf. < 727C
0.7
6
0.0
22
Adapted from Fig. 10.28,Callister & Rethwisch 3e. (Fig. 10.28 adapted from Binary Alloy Phase Diagrams, 2nd ed., Vol. 1, T.B. Massalski (Ed.-in-Chief), ASM International, Materials Park, OH, 1990.)
64
The Fe-Fe3C Eutectoid Transformation
Coarse pearlite formed at higher temperatures – relatively soft
Fine pearlite formed at lower temperatures – relatively hard
• Transformation of austenite to pearlite:
Adapted from Fig. 10.15, Callister & Rethwisch 3e.
pearlite growth direction
Austenite ()grain boundary
cementite (Fe3C)
Ferrite ()
• For this transformation, rate increases with [Teutectoid – T ] (i.e., T).
Adapted from Fig. 11.12, Callister & Rethwisch 3e.
675°C (T smaller)
0
50
y (%
pea
rlite
)600°C
(T larger)650°C
100
Diffusion of C during transformation
Carbon diffusion
65
Adapted from Fig. 11.13,Callister & Rethwisch 3e. (Fig. 11.13 adapted from H. Boyer (Ed.) Atlas of Isothermal Transformation and Cooling Transformation Diagrams, American Society for Metals, 1977, p. 369.)
Generation of Isothermal Transformation Diagrams
• The Fe-Fe3C system, for Co = 0.76 wt% C• A transformation temperature of 675°C.
100
50
01 102 104
T = 675°C
y,
% tr
ansf
orm
ed
time (s)
400
500
600
700
1 10 102 103 104 105
0%pearlite
100%
50%
Austenite (stable) TE (727C)Austenite (unstable)
Pearlite
T(°C)
time (s)
isothermal transformation at 675°C
Consider:
66
• Eutectoid composition, C0 = 0.76 wt% C• Begin at T > 727°C• Rapidly cool to 625°C• Hold T (625°C) constant (isothermal treatment)
Adapted from Fig. 11.14,Callister & Rethwisch 3e. (Fig. 11.14 adapted from H. Boyer (Ed.) Atlas of Isothermal Transformation and Cooling Transformation Diagrams, American Society for Metals, 1997, p. 28.)
Austenite-to-Pearlite Isothermal Transformation
400
500
600
700
0%pearlite
100%
50%
Austenite (stable)TE (727C)
Austenite (unstable)
Pearlite
T(°C)
1 10 102 103 104 105
time (s)
67
10 103 105
time (s)10-1
400
600
800
T(°C)Austenite (stable)
200
P
B
TE
0%
100%
50%
A
A
Bainite: Another Fe-Fe3C Transformation Product • Bainite: -- elongated Fe3C particles in -ferrite matrix -- diffusion controlled • Isothermal Transf. Diagram,
C0 = 0.76 wt% C
Adapted from Fig. 11.18, Callister & Rethwisch 3e.
Adapted from Fig. 11.17, Callister & Rethwisch 3e. (Fig. 11.17 from Metals Handbook, 8th ed., Vol. 8, Metallography, Structures, and Phase Diagrams, American Society for Metals, Materials Park, OH, 1973.)
Fe3C(cementite)
5 m
(ferrite)
100% bainite
100% pearlite
68
• Spheroidite: -- Fe3C particles within an -ferrite matrix -- formation requires diffusion -- heat bainite or pearlite at temperature
just below eutectoid for long times -- driving force – reduction
of -ferrite/Fe3C interfacial area
Spheroidite: Another Microstructure for the Fe-
Fe3C System
Adapted from Fig. 11.19, Callister & Rethwisch 3e. (Fig. 11.19 copyright United States Steel Corporation, 1971.)
60 m
(ferrite)
(cementite)
Fe3C
69
• Martensite: -- (FCC) to Martensite (BCT)
Adapted from Fig. 11.22, Callister & Rethwisch 3e. (Fig. 11.22 courtesy United States Steel Corporation.)
Adapted from Fig. 11.21, Callister & Rethwisch 3e.
Martensite: A Nonequilibrium Transformation Product
Martensite needlesAustenite
60
m
xx x
xx
xpotential C atom sites
Fe atom sites
Adapted from Fig. 11.23, Callister & Rethwisch 3e.
• Isothermal Transf. Diagram
• to martensite (M) transformation.. -- is rapid! (diffusionless) -- % transf. depends only on T to
which rapidly cooled
10 103 105 time (s)10-1
400
600
800
T(°C)Austenite (stable)
200
P
B
TE
0%
100%50%
A
A
M + AM + A
M + A
0%50%90%
70
(FCC) (BCC) + Fe3C
Martensite Formationslow cooling
tempering
quench
M (BCT)
Martensite (M) – single phase
– has body centered tetragonal (BCT) crystal structure
Diffusionless transformation BCT if C0 > 0.15 wt% C
BCT few slip planes hard, brittle
Austenite Ferrite + Cementite = Pearlite
Tempered Martensite
71
Phase Transformations of AlloysEffect of adding other
elementsChange transition temp.
Cr, Ni, Mo, Si, Mn
retard + Fe3C
reaction (and formation of
pearlite, bainite)
Adapted from Fig. 11.24, Callister & Rethwisch 3e.
Chapter 09: Phase Diagram 72
Chapter 09: Phase Diagram 73
Problem:
For Pb-Sn system at 150°C, calculate relative amounts of
each phase by (a) Mass fraction (b) Volume fraction
0.6711994099
CC
CCW
n(a)Solutio
gm/cm 7.3:ρgm/cm 11.2:ρ
:Given
αβ
1βα
3β
3α
Chapter 09: Phase Diagram 74
Problem: Continue ….
33
33
αβ
α1β
cm 4.52gm/cm 7.3
gm 33)(
v
cm 5.98gm/cm 11.2
gm 67)(
v
Fraction Volume (b) Solution
0.3311991140
CC
CCW
1-0.67=0.33
Chapter 09: Phase Diagram 75
0.434.525.98
4.52vv
vV
0.574.525.98
5.98vv
vV
Fraction Volume
βα
ββ
βα
αα
Problem: Continue ….
Vα is volume fraction of the alpha phase, Vα and Vβ denote the volumes of the respective phases in the alloy.