Material Engineering - Lecture - Phase Diagrams, Lecture notes of Material Engineering

Detail Summery about Phase Diagrams, Introduction, Solubility Limits, Phase Equilibrium, Interpretation of Phase Diagrams, Mechanical Properties.

Typology: Lecture notes

2010/2011

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Phase Diagrams

Chapter 10 (part 1)

Introduction

  • (^) Solubility Limits

Phases

Phase Equilibrium

  • (^) Interpretation of Phase Diagrams

Binary Isomorphous Systems (Cu-Ni)

Development of Microstructure

  • (^) Mechanical Properties

Binary Eutectic Systems

Development of Eutectic Alloy Microstructure

Phase Equilibria: Solubility Limit

  • Solution – solid, liquid, or gas solutions, single phase
  • Mixture – more than one phase

Question: What is the

solubility limit for sugar in
water at 20 °C?

Answer: 65 wt% sugar.

At 20°C, if C < 65 wt% sugar: syrup

At 20°C, if C > 65 wt% sugar: syrup + sugar

  • Solubility Limit:
Maximum concentration for
which only a single phase
solution exists.
Sugar/Water Phase Diagram

Sugar

Temperature (°C)

C = Composition (wt% sugar)

L

(liquid solution

i.e., syrup)

Solubility

Limit

L

(liquid)

S

(solid

(^20) sugar)

Water

Equilibrium

A system is at equilibrium if its free energy is at a

minimum, given a specified combination of

temperature, pressure and composition.

The (macroscopic) characteristics of the system

do not change with time — the system is stable.

  • (^) A change in T, P or C for the system will result in

an increase in the free energy and possible

changes to another state whereby the free

energy is lowered.

7

Phase Diagrams

  • Indicate phases as a function of Temp, Comp and Pressure.
  • Focus on:
    • binary systems: 2 components.
    • independent variables: T and C (P = 1 atm is almost always used).
Cu-Ni
system
  • 2 phases:
L

(liquid)

(FCC solid solution)

  • 3 different phase fields:

L

L + 

wt% Ni

T(°C)

L (liquid)

(FCC solid

solution)

L

liquidus

solidus

  • Changing T can change # of phases: path A to B.
  • Changing C o can change # of phases: path B to D.

Effect of Temperature & Composition (C

o

wt% Ni 0 20 40 60 80 100

T(°C)

L (liquid)

(FCC solid solution)

L

liquidus

solidus

A
B
D

Cu

Cu-Ni
system
  • Rule 2: If we know T and C o

, then we know:

--the composition of each phase.
  • Examples:
wt% Ni

20

1200

1300

T(°C)
L (liquid)
(solid)

30 40 50

T
A
A
D
TD
TB
B

tie line

CLCo
C
Cu-Ni
system

Phase Diagrams: composition of phases

At T

A

= 1320°C:
Only Liquid (L) present
C

L

= C

0

( = 35 wt% Ni)
At T

B

= 1250°C:
Both

and L present
At T

D

= 1190°C:
Only Solid () present
C

= C

0

( = 35 wt% Ni)
C

L

= C
liquidus
( = 32 wt% Ni)
C

= C
solidus
( = 43 wt% Ni)
  • Rule 3: If we know T and C o

, then we know:

--the amount of each phase (given in wt%).
Cu-Ni system
  • Examples:
At T
B
: Both  and L
At T
A
: Only Liquid (L)
W
L
= 100wt%, W
At T
D
: Only Solid ()
W
L
= 0, W
= 100wt%
C
o
= 35wt%Ni
wt% Ni

20

1200

1300

T(°C)
L (liquid)
(solid)

30 40 50

T
A
A
D
TD
TB
B

tie line

CLCo
C
R S

Phase Diagrams: weight fractions of phases

W

L

S

R

S

W 

R

R

S

 73 wt%

R

R

S

S

R

 S

W

L

C

 C

o

C

 C

L

= 27wt %

R

R

S

W

C

o

 C

L

C

 C

L

W

L

S

R

S

W 

R

R

S

  • Development of

microstructure during

the non-equilibrium

solidification of a 35 wt

% Ni-65 wt% Cu alloy

outcome:

  • (^) Segregation-

nonuniform distribution

of elements within

grains.

  • Weaker grain

boundaries if alloy is

reheated.

  • C 

changes as it solidifies.

  • Cu-Ni case:
  • Fast rate of cooling:

Cored structure

  • Slow rate of cooling:

Equilibrium structure

First  to solidify has C

= 46wt%Ni.
Last  to solidify has C

= 35wt%Ni.

First  to solidfy:

46wt%Ni

Uniform C  :

35wt%Ni

Last  to solidfy:

< 35wt%Ni

Cored vs Equilibrium Phases

  • (^) Coring can be eliminated by means of a homogenization heat treatment carried out at

temperatures below the alloy’s solidus. During the process, atomic diffusion produces grains

that are compositionally homogeneous.

Binary Isomorphous Systems

Cu-Ni system:

The liquid L is a homogeneous liquid solution composed of

Cu and Ni.

  • (^) The α phase is a substitutional solid solution consisting of

Cu and Ni atoms with an FCC crystal structure.

  • (^) At temperatures below 1080 C, Cu and Ni are mutually

soluble in each other in the solid state for all compositions.

  • (^) The complete solubility is explained by their FCC structure,

nearly identical atomic radii and electro-negativities, and

similar valences.

  • (^) The Cu-Ni system is termed isomorphous because of this

complete liquid and solid solubility of the 2 components.

Cu-Ni
phase
diagram

Isomorphous Binary Phase Diagram

  • Phase diagram:

Cu-Ni system.

  • System is:

-- binary

2 components:
Cu and Ni.

-- isomorphous

i.e., complete
solubility of one
component in
another;  phase
field extends from
0 to 100 wt% Ni.

wt% Ni 0 20 40 60 80 100

T(°C)

L (liquid)

(FCC solid

solution)

L

liquidus

solidus

Importance of Phase Diagrams

  • There is a strong correlation between

microstructure and mechanical properties,

and the development of alloy

microstructure is related to the

characteristics of its phase diagram.

  • Phase diagrams provide valuable

information about melting, casting,

crystallization and other phenomena.