13
CHAPTER 2 (CONTD.) Slow Cooling of an Isomorphous Alloy Rapid Cooling of an Isomorphous Alloy Binary Eutectic System MTE/III SEMESTER/MSE/MTE 2101 1

Two Component System

Embed Size (px)

Citation preview

Page 1: Two Component System

MTE/III SEMESTER/MSE/MTE 2101 1

CHAPTER 2 (CONTD.)

Slow Cooling of an Isomorphous Alloy Rapid Cooling of an Isomorphous Alloy Binary Eutectic System

Page 2: Two Component System

MTE/III SEMESTER/MSE/MTE 2101 2

SLOW COOLING OF AN ISOMORPHOUS ALLOY

Also, called as Equilibrium Cooling. Let us consider Cu-Ni system 35 wt% Ni–65 wt% Cu. At 1300° C; point a, the alloy is completely liquid. As cooling begins, no microstructural or compositional

changes will be realized until we reach the liquidus line.

At 1260°C; point b, the first solid α begins to form, which has a composition dictated by the tie line drawn at this temperature i.e., 46 wt% Ni–54 wt% Cu.

With continued cooling, both compositions and relative amounts of each of the phases will change.

The fraction of α phase will increase.

Pic Courtesy: Material Science and Engineering, Callister.

Page 3: Two Component System

MTE/III SEMESTER/MSE/MTE 2101 3

At 1250°C, point c, the compositions of the liquid and α phases are 32 wt% Ni–68 wt% Cu [L(32 Ni)] and 43 wt% Ni–57 wt% Cu [ (43 Ni)].

The solidification process is virtually complete at1220°C about point d; the composition of the solid is approximately 35 wt% Ni–65 wt% Cu.

Upon crossing the solidus line, this remaining liquid solidifies; the final product then is a polycrystalline -phase solid solution that has a uniform 35 wt% Ni–65 wt% Cu composition at point e.

Pic Courtesy: Material Science and Engineering, Callister.

Page 4: Two Component System

MTE/III SEMESTER/MSE/MTE 2101 4

RAPID COOLING OF AN ISOMORPHOUS ALLOY

Also, called as Non Equilibrium Cooling. Let us consider Cu-Ni system 35 wt% Ni–65 wt

% Cu. At 1300° C; point a´, the alloy is completely

liquid. As cooling begins, no microstructural or

compositional changes will be realized until we reach the liquidus line.

At point b´, (approximately 1260°C), α-phase particles begin to form, which, from the tie line constructed, have a composition of 46 wt% Ni–54 wt% Cu [ (46 Ni)].

Pic Courtesy: Material Science and Engineering, Callister.

Page 5: Two Component System

MTE/III SEMESTER/MSE/MTE 2101 5

Upon further cooling to point c´ (about 1260°C ), the liquid composition has shifted to 29 wt% Ni–71 wt% Cu; furthermore, at this temperature the composition of the αphase that solidified is 40 wt% Ni–60 wt% Cu [ (40 Ni)].

Because of the rapid cooling, the solidus line shifted (indicated in dashed line) and solid composition has increased.

At point d´ (temperature 1220°C), the solidification should complete but there is still little amount of liquid is left.

Pic Courtesy: Material Science and Engineering, Callister.

Page 6: Two Component System

MTE/III SEMESTER/MSE/MTE 2101 6

The solidification should be completed at point e´ in comparison to slow cooling but since there is a shift in the solidus line, solidification process takes longer time than usual.

It completes at point e´ (temperature 1205°C).

Pic Courtesy: Material Science and Engineering, Callister.

Page 7: Two Component System

MTE/III SEMESTER/MSE/MTE 2101 7

PHENOMENA OF SEGREGATION TAKES PLACE WHICH IS NOTHING BUT NON-UNIFORM DISTRIBUTION OF GRAINS.

Slow Cooling Rapid Cooling

Page 8: Two Component System

BINARY EUTECTIC SYSTEMS

Another type of common and relatively simple phase diagram found for binary alloys for the copper–silver system; this is known as a binary eutectic phase diagram.

MTE/III SEMESTER/MSE/MTE 2101 8

Pic Courtesy: Material Science and Engineering, Callister

Page 9: Two Component System

Features of Phase Diagram Three single-phase regions are found on

the diagram: α,β and liquid. α phase: Cu rich solid solution, solute is

Ag, FCC structure. β phase: Ag rich solid solution, solute is

Cu, FCC structure. Pure copper and pure silver are also

considered to be α and β phases.

MTE/III SEMESTER/MSE/MTE 2101 9

Page 10: Two Component System

Features of Phase Diagram (Contd.) The solubility in each of these solid phases is

limited, in that at any temperature below line BEG only a limited concentration of silver will dissolve in copper (for the α phase) similarly for copper in silver (for the β phase).

The solubility limit for the α phase corresponds to the boundary line, labelled CBA, between the α/(α+β) and α/(α+L) phase regions; it increases with temperature to a maximum [8.0 wt% Ag at 779°C] at point B and decreases back to zero at the melting temperature of pure copper, point A 1085°C.

MTE/III SEMESTER/MSE/MTE 2101 10

Page 11: Two Component System

Features of Phase Diagram (Contd.) The solid solubility limit line separating

the α and (α+β) phase regions is termed a solvus line; the boundary AB between the α and (α+L) fields is the solidus line.

MTE/III SEMESTER/MSE/MTE 2101 11

Page 12: Two Component System

Features of Phase Diagram (Contd.) There are also three two-phase regions found for the

copper–silver system: α + L, β+L, α+β. As silver is added to copper, the temperature at

which the alloys become totally liquid decreases along the liquidus line, line AE; thus, the melting temperature of copper is lowered by silver additions.

The same can be said for silver, as copper is added to silver, the temperature of copper reduces complete melting along the other liquidus line, FE..

These liquidus lines meet at the point E on the phase diagram, through which also passes the horizontal isotherm line BEG.

Point E is called an invariant point.

MTE/III SEMESTER/MSE/MTE 2101 12

Page 13: Two Component System

Features of Phase Diagram (Contd.) An important reaction occurs for an alloy of

composition CE as it changes temperature TE; in passing through this reaction may be written as follows:

The reaction occurring at Point E along line BEG is called as “Eutectic Reaction”.

MTE/III SEMESTER/MSE/MTE 2101 13