Ch-7 Compatibility Mode

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    CHAPTER 7

    Chapter 9-

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    Contents of Todays Lecture

    Introduction to phase change processes. Phase diagram.

    Chapter 9-

    conditions of solubilities.

    Lever Rule.

    Fe-C phase diagram.

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    Introduction to phase diagrams

    Most of the engineering materials are alloys. In a poly-phase material, the overall properties

    depend upon Number of hases resent

    Chapter 9-

    Relative amount of each phase Composition and microstructure of each phase

    Size and distribution of the phases in the microstructure.

    In this topic we are going to develop theunderstanding of composition-structure-property relationship of materials.

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    About Phase diagram

    The phase diagram or Equilibrium diagram is the

    graphical representation of number of phases that arepresent, their compositions and the relative amount ofeach phase as the functions of temperature and theoverall composition of the material.

    Chapter 9-

    The term equilibrium denotes a state of rest whichimplies that, for a given composition and temperature,there shall not be any change in the constituents withtime.

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    Solid solution.

    Solid Solution: When two elements dissolvein the solid state, the resulting phase iscalled as solid solution.

    Chapter 9-

    There are following possibilities The metals are completely soluble in solid

    state.

    The metals are completely insoluble in solidstate.

    The metals are partially soluble in solid

    state.

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    System The universe or any part of it.

    Phase A region in the system that has a distinct structure and/or

    composition

    Structure How the atoms or molecules of the components are physically

    arranged in space

    Composition The relative amounts of different components

    Components Chemically distinct species, generally pure elements or

    compounds

    Phase Diagram Vocabulary

    Chapter 9-

    Phase Diagram A graphical representation of the influence of various factors,such as temperature, pressure, and composition on the phases

    that exist in a system.

    Unary System A system that has only one component

    Binary System A system that has two components what this courseprimarily deals with

    Ternary System A system that has three components

    Quaternary System A system that has four components

    A, B, C Generic names of componentsL, , , Generic names of phases

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    Material Science & Engineering

    Processing Structure Properties Performance

    Chapter 9-

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    What is materials science and

    engineering?

    Materials science is the investigation of therelationships that exist between the

    structure and ro erties of materials.

    Chapter 9-

    Materials engineering uses the structure-

    property relationships of materials to link

    processing withperformance.

    Processing Structure Properties Performance

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    Whats meant by the structure of a

    material?

    Subatomic- Interactions of electrons with anucleus

    Atomic- Arrangement of atoms relative to

    Chapter 9-

    each other Microscopic- Organization of large groups

    of atoms (can be seen with a microscope)

    Macroscopic- Structure that can beobserved with the naked eye.

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    Example: Snow.

    Chapter 9-

    Individualmolecules arearranged into

    crystals

    Individualcrystals form

    a solidstructure

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    .is a lot like metal

    Chapter 9-

    Individualatoms are

    arranged intograins

    Individualgrains form

    a solidstructure

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    TerminologyTerminologyTerminologyTerminology

    Chapter 9-

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    SYSTEM

    SYSTEM

    Chapter 9-

    SURROUNDING

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    Components (C)Components (C)Components (C)Components (C)No. of Elements or Compounds thatNo. of Elements or Compounds thatNo. of Elements or Compounds thatNo. of Elements or Compounds that

    constitute a systemconstitute a systemconstitute a systemconstitute a system

    1-C

    Chapter 9-

    -

    3-C

    4-C

    Multi-C

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    PhasePhasePhasePhase Physically distinct,

    Mechanically Separable &

    Chemically homogeneous

    Chapter 9-

    Region of a system is called as phase.

    Homogeneous portion of a system that has

    uniform physical and chemical characteristics is

    called as a PHASE

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    Solid

    Various phases [e.g. crystal structures (diamond; graphite)

    Alloys (sometimes its difficult to tell this - microscopic

    examination may be necessary {dispersions uniform onmacroscopic scale}) Miscible one phase (P=1)

    Chapter 9-

    Liquid Miscible liquids are one phase

    Immiscible liquids are multiple phases (P>1)

    Gas

    Systems consisting of gases can have only one phase

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    Definitions

    Heterogeneous and homogeneous systems

    Systems with one phase are homogeneous

    Systems with more than one phase are heterogeneous

    Constituent- a chemical species (ion or molecule which ispresent

    Component (C) - chemically independent constituents of a

    Chapter 9-

    C = #of independent chemical constituents - # ofdistinct chemical reactions #of independent chemical constituents = total # of constituents

    minus the number of any restrictive conditions (chargeneutrality, material balance etc.)

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    (lighterphase)

    Solid PhaseSolid PhaseSolid PhaseSolid PhaseCOMPONENTS AND PHASES

    Chapter 9- 33

    AlAlAlAl----CuCuCuCu

    AlloyAlloyAlloyAlloy

    ar er

    phase)

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    EquilibriumEquilibriumEquilibriumEquilibrium

    State of a System at specified conditionswhen the system possesses minimum free

    ener

    Chapter 9-

    Temperature, Pressure & Composition

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    PHASE EQUILIBRIUMPHASE EQUILIBRIUMPHASE EQUILIBRIUMPHASE EQUILIBRIUM

    Constancy with time in physicalcharacteristics

    Chapter 9-

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    Gibbs Phase RuleGibbs Phase RuleGibbs Phase RuleGibbs Phase Rule For a solid solution, the phase rule is

    {P + F = C + N

    }

    P No. of Phases

    Chapter 9-

    F DOF

    CNo. of Components

    N Non-compositional variables

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    Degree of Freedom (DOF)Degree of Freedom (DOF)Degree of Freedom (DOF)Degree of Freedom (DOF)

    The number of independent variables

    required to describe the state of a system is

    called as the DOF

    Chapter 9-

    Externally controlled variables

    (Temp, Pressure, Composition)

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    Gibbs Phase RuleGibbs Phase RuleGibbs Phase RuleGibbs Phase Rule Ex. Ice + Water, heating at constant pressure

    {P + F = C + N

    }

    P No. of PhasesP + F = 1 + 1

    Chapter 9-

    F DOF

    CNo. of Components

    N Non-compositional variables

    F = 2 - P

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    One Component Systems

    Phase rule says that you can have at most 3 phasesF = C- P +2; C=1 so F=3-P

    If P=3, F=0 system is invariant Specified by temperature and pressure and occurs at 1 point

    (called the triple point)

    If one phase is present, F = 2 that is P and T can be varied

    Chapter 9-

    n epen en y

    This defines an area in a P,T diagram which only onephase is present

    If two phases are present, F = 1 so only P or T can bevaried independently.

    This defines a line in a P, T diagram

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    Solubility LimitSolubility LimitSolubility LimitSolubility Limit

    The elements or compounds which are

    mixed

    Chapter 9-

    Solvent SoluteAt some specific temperature there is a maximum concentration

    of solute atoms that may dissolve in the solvent to form a solid

    solution this is called solubility limit

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    erature

    (C)

    Lli uid solution

    SolubilityLimit L

    (liquid)+60

    80

    100

    THE SOLUBILITY LIMIT

    Chapter 9- 2

    Pure

    Sugar

    Temp

    0 20 40 60 80 100Co=Composition (wt% sugar)

    i.e., syrup)

    (solidsugar)

    65

    20

    Pure

    Water

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    Changing T can change # of phases: path A to B.

    Changing Co can change # of phases: path B to D.

    )

    B(100,70)1 phase

    100

    D(100,90)2 phases

    EFFECT OF T & COMPOSITION (Co)

    Chapter 9-

    70 80 1006040200

    Tem

    perature(

    Co=Composition (wt% sugar)

    L(liquid solution

    i.e., syrup)

    A(70,20)2 phases

    20

    40

    60

    0

    (liquid)+S

    (solidsugar)

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    PhasePhasePhasePhase----EquilibriumEquilibriumEquilibriumEquilibrium

    Chapter 9-

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    Phase DiagramsPhase DiagramsPhase DiagramsPhase Diagrams

    1-Component

    2-Components

    3-Components

    Chapter 9-

    Unary P.D. (Binary P.D.) (Ternary P.D.)

    Much of the information about the control of microstructure or

    phase structure of a particular alloy system is conveniently and

    concisely displayed in what is called a phase diagram, also

    often termed as equilibrium or constitutional diagram.

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    Unary Phase Diagram (Fe)

    GAS

    LIQUID

    3000

    1535

    P + F = C + N

    P + F = 1 + 2

    F = 3 - P

    Chapter 9-Pressure (GPa)

    Temp (oC)

    FCC ()

    HCP ()

    BCC ()

    BCC ()

    1410

    910

    For s ngle P,F = 2

    For two P,

    F = 1

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    BINARY ISOMORPHOUS DIAGRAMBINARY ISOMORPHOUS DIAGRAMBINARY ISOMORPHOUS DIAGRAMBINARY ISOMORPHOUS DIAGRAM

    Cu + NiCu + NiCu + NiCu + Ni

    Chapter 9-

    100 % Liquid solubility and100 % Liquid solubility and100 % Liquid solubility and100 % Liquid solubility and100 % Solid solubility100 % Solid solubility100 % Solid solubility100 % Solid solubility

    PHASE DIAGRAM f C Ni

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    1400

    1500

    1600

    T(C)

    L (liquid)

    qu

    idus

    PHASE DIAGRAM for Cu-Ni

    1453 C

    Chapter 9- 5

    20 40 60 80 10001000

    1100

    1200

    (FCC solidsolution)

    L

    solidu

    (Cu) (Ni)

    1085 C

    COMPOSITION WT %

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    InterpretationInterpretationInterpretationInterpretationof Phase Diagramsof Phase Diagramsof Phase Diagramsof Phase Diagrams

    1. Phases Present

    Chapter 9-

    2. Composition of Phases

    3. Weight Fraction of Phases

    T(C) Phases PresentPhases PresentPhases PresentPhases Present

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    1400

    1500

    1600T(C)

    L (liquid)

    liquidu

    s

    solidus

    1250,35)

    Phases PresentPhases PresentPhases PresentPhases Present

    Chapter 9- 6

    wt% Ni20 40 60 80 1000

    1000

    1100

    1200(FCC solidsolution)

    L

    A(1100,60)

    B

    composition of phasescomposition of phasescomposition of phasescomposition of phases

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    1300

    T(C)

    L (liquid)liq

    uidus

    olidu

    s

    TAA

    B

    tie line

    L+

    composition of phasescomposition of phasescomposition of phasescomposition of phases

    1280 C

    1320C

    Chapter 9- 7

    wt% Ni

    20

    1200

    (solid)L+

    30 40 50

    DTD

    433532

    CoCL C

    weight fractions of phases

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    1300

    T(C)

    L (liquid) liquid

    us

    solid

    us

    TA A

    TBB

    tie line

    L+

    weight fractions of phases

    Chapter 9- 8

    wt% Ni

    20

    1200

    (solid)L+

    30 40 50

    DTD

    433532C

    oC

    LC

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    CoR S

    CL C

    THE LEVER RULE

    Chapter 9- 9

    WWL

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    WL= S/(R+S) WL= (C-C0)/(C-CL)

    Chapter 9-

    W = (C0-CL)/(C-CL)

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    Volume Fraction of Phases

    Chapter 9-

    Relation in between

    Volume and Weight Fraction

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    Equilibrium COOLING IN A Cu-Ni

    Chapter 9-

    COOLING IN A Cu Ni BINARY

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    COOLING IN A Cu-Ni BINARY

    Equilibrium Cooling

    System is:Binaryi.e., 2 components:

    Chapter 9-

    u an .

    Isomorphousi.e., complete solubility of one

    component in another; phase

    field extends from 0 to 100wt% Ni.

    Extreme slow cooling of alloy

    EX: COOLING IN A Cu-Ni BINARY

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    1300

    L (liquid)

    L+

    T(C)

    A

    D

    B

    L: 35wt%Ni

    : 46wt%Ni

    C

    L: 35wt%Ni

    4643

    32

    24

    35

    L: 32wt%Ni

    EX: COOLING IN A Cu Ni BINARY

    Chapter 9-10wt% Ni20

    1200

    30 40 501100

    (solid)

    L+

    35Co

    E : 43wt%NiL: 24wt%Ni

    : 36wt%Ni

    COOLING IN A Cu-Ni BINARY

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    COOLING IN A Cu-Ni BINARY

    Non-Equilibrium Cooling

    System is:Binary

    Chapter 9-

    .e., componen s:

    Cu and Ni.

    Isomorphousi.e., complete solubility of one

    component in another; phasefield extends from 0 to 100wt% Ni.

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    Non-Equilibrium COOLING IN A

    -

    Chapter 9-

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    Chapter 9-

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    NonNonNonNon----Equilibrium CoolingEquilibrium CoolingEquilibrium CoolingEquilibrium Cooling

    Consequences of Non-Equilibrium cooling

    Chapter 9-

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    C changes as we solidify.

    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.

    Uniform C:

    CORED VS EQUILIBRIUM PHASES

    Chapter 9-

    46wt%Ni

    35wt%Ni

    Last to solidfy:

    < 35wt%Ni

    MECHANICAL PROPERTIES: Cu-Ni System

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    Effect of solid solution strengthening

    on:--Tensile strength (TS) --Ductility (%EL,%AR)

    MECHANICAL PROPERTIES: Cu-Ni System

    on(%EL)

    50

    60

    %EL forpure Ni

    %EL for pure Cu

    ngth(MP

    a)

    400

    TS for

    Chapter 9-

    Elong

    at

    Com osition, wt%Ni

    Cu Ni0 20 40 60 80 100

    20

    30

    TensileSt

    re

    Composition, wt%Ni

    Cu Ni0 20 40 60 80 100

    200

    300pure

    TS for pure Cu

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    Binary Eutectic SystemsBinary Eutectic SystemsBinary Eutectic SystemsBinary Eutectic Systems

    Chapter 9-

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    Binary Eutectic System

    Apply Modified Gibbs Phase Rule Phases present: L, and (P=3)

    Components: Pb and Sn (C=2)

    Chapter 9-

    P+F=C+1

    F=0 no degrees of freedom

    Therefore, three phases can coexist in a binary system

    only at a unique temperature and for unique

    compositions of the three phases

    Upon cooling, there is a temperature arrest during the

    solidification process (eutectic reaction)

    T(C)BINARY-EUTECTIC SYSTEMS

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    L (liquid)

    L + L+

    1200( )

    600

    800

    1000

    TE 8.0 71.9 91.2779C

    A

    B E G

    Solidus

    line F

    Chapter 9-13

    +

    Co, wt% Ag20 40 60 80 1000

    200

    400

    CE

    C

    o vus ne

    H

    EX: Pb-Sn EUTECTIC SYSTEM

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    L + L+ 200

    T(C)

    300

    L (liquid)

    represents a solid solution of tin in lead

    For tin is a solvent and lead is a solute

    Chapter 9-14

    +

    18.3

    Co, wt% Sn

    20 40 60 80 1000Co

    100

    61.9 97.8150

    Wh d l k k ?

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    What we wd like to know?

    Microstructure Com osition

    Chapter 9-

    Weight Fraction

    EX: Pb-Sn EUTECTIC SYSTEM

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    L + L+ 200

    T(C)

    300

    L (liquid)

    183C

    Chapter 9-15

    +

    18.3

    Co, wt% Sn

    20 40 60 80 1000Co

    100

    61.9 97.8150

    11 99

    R S

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    Amounts of Phases at different temperatures

    QP

    PW

    QP

    QW

    L+

    =

    +=

    At Teutectic + T

    ( )

    QP

    PW

    QP

    QW

    L

    cproeutecti

    +=

    +=

    Chapter 9-

    eutectic -

    ( )

    RQP

    PW

    RQP

    RQW

    total

    ++

    =

    ++

    +=

    ( ) ( ) ( )cproeutectitotaleutectic

    WWW =

    MICROSTRUCTURES IN EUTECTIC SYSTEMS

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    L +

    T(C)

    300 L

    L: Co

    wt%Sn

    L

    400

    solidus Liquidus

    Chapter 9-16

    Co, wt% Sn10

    2

    200Co

    100

    30

    : Co

    wt%Sn

    +

    (room T solubility limit)

    TE-

    System)

    MICROSTRUCTURES IN EUTECTIC SYSTEMS

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    2wt%Sn < Co < 18.3wt%Sn

    Result:-- polycrystal with fine

    crystals.

    L +

    T(C)

    300

    L

    L: Cowt%Sn

    400

    L

    d

    Chapter 9-17

    o

    200

    Co, wt% Sn10

    18.3

    200Co

    100

    30

    +

    (sol. limit at TE)

    TE

    2(sol. limit at Troom)

    solvus

    f

    g

    MICROSTRUCTURES

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    T(C)

    300

    L: Cowt%Sn

    Micrograph of Pb-Sneutecticmicrostructure

    Co = CE Result: Eutectic microstructure

    --alternating layers of and crystals.

    IN EUTECTIC SYSTEMS

    Chapter 9-18

    L + 200

    Co

    , wt% Sn

    20 400

    100

    60

    +

    TE

    : 18.3wt%Sn

    080 100

    L +

    CE18.3 97.8

    61.9

    183C

    : 97.8wt%Sn 160m

    Pb-Sn

    system

    MICROSTRUCTURES

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    T(C)

    300 L

    L: Cowt%Sn

    L

    L

    18.3wt%Sn < Co < 61.9wt%Sn

    Result: crystals and a eutectic microstructure

    Just above TE:C= 18.3wt%Sn

    CL = 61.9wt%Sn

    IN EUTECTIC SYSTEMS

    Chapter 9-

    L +

    200

    Co, wt% Sn

    20 400

    100

    60

    +

    TE

    080 100

    L +

    Co18.3 61.9

    primary

    97.8

    S

    S

    R

    R

    eutectic eutectic

    19

    -

    system WL= (1-W) =50wt%R+ S

    W = =50wt%

    Just below TE:

    C = 18.3wt%Sn

    C= 97.8wt%SnS

    R+ SW = =73wt%

    W= 27wt%

    HYPOEUTECTIC & HYPEREUTECTIC

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    T(C)

    (Pb-Sn

    System)

    L + 200

    Co, wt% Sn20 400

    300

    100

    L

    60

    +

    TE

    080 100

    L +

    Cohypoeutectic

    Cohypereutectic

    HYPOEUTECTIC & HYPEREUTECTIC

    Chapter 9-20

    18.3

    61.9

    97.8eutectic

    hypereutectic: (illustration only)

    160m

    eutectic: Co=61.9wt%Sn

    175m

    hypoeutectic: Co=50wt%Sn

    eutectic micro-constituent

    IRON-CARBON (Fe-C) PHASE DIAGRAM

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    ite)

    1600

    1400

    1200

    L

    (austenite)

    +L L+Fe3C

    1148C A

    SR

    Chapter 9-21

    Fe3C

    (ceme

    n1000

    800

    600

    4000 1 2 3 4 5 6 6.7

    +Fe3C

    +Fe3C

    +

    (Fe) C wt% C0.77 4.30

    727C = TeutectoidB

    R S

    Important Points of to study Fe-C Diagram

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    1. Pure Iron (0% C)

    2. Cementite (Fe3C) (6.70% of C)

    3. Alpha Ferrite4. Austenite

    Chapter 9-

    .

    6. Cementite7. Reactions (Eutectic and Eutectoid)

    8. Ferrous alloy

    9. Eutectoid Alloy

    10. Hypo-Eutectoid Alloy

    11. Hyper-Eutectoid Alloy

    IRON-CARBON (Fe-C) PHASE DIAGRAM

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    2 importantpoints

    -Eutectic (A):

    -Eutectoid (B):

    L +Fe3C

    +Fe3C

    ementite)

    1600

    1400

    1200

    1000

    L

    (austenite)

    +L

    +Fe3C

    L+Fe3C

    1148C

    T(C)

    A

    SR

    IRON-CARBON (Fe-C) PHASE DIAGRAM

    Chapter 9-21

    Result: Pearlite =

    alternating layers of and Fe3C phases.

    120m

    Fe3C

    (c

    600

    4000 1 2 3 4 5 6 6.7

    +Fe3C

    (Fe) Co, wt% C0.77 4.30

    = eutectoid

    R S

    Fe3C (cementite-hard)

    (ferrite-soft)

    Ceutec

    toid

    Iron-Carbon System

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    Reactions on

    cooling

    Peritectic

    L +

    Chapter 9-

    Eutectic

    L + Fe3C

    Eutectoid

    + Fe3C

    Steel Cast Iron

    Iron-Carbon or Iron-Fe3C

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    In principle, the components of the phase diagram should beiron (Fe) and carbon/graphite (C). Fe and C form an intermediate compound Fe3C, which is very stable

    There isnt anything of interest at carbon contents greater than 25 at.%

    or 6.7 wt.% C. Fe3C is considered to be a component, and the binary phase diagram is

    drawn using Fe and Fe3C.

    Chapter 9-

    Ferrite iron bcc structure Austenite iron fcc structure

    High temperature iron bcc structure

    Cementite Fe3C

    Steels have carbon contents

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    Cabon ALLOYS

    Chapter 9-

    HYPOEUTECTOID STEEL

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    HYPOEUTECTOID STEEL

    Chapter 9-22

    HYPEREUTECTOID STEEL

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    HYPEREUTECTOID STEEL

    Chapter 9-23

    ALLOYING STEEL WITH MORE ELEMENTS

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    tectoid(

    C)

    Ti

    800

    1000

    1200

    Mo

    Si

    W

    Crtectoid(

    wt%C)

    Ni

    0.4

    0.6

    0.8

    Cr

    Si

    Teutectoid changes: Ceutectoid changes:

    Chapter 9-

    T

    Eu

    wt. % of alloying elements

    Ni600

    0 4 8 12

    Mn

    wt. % of alloying elements

    C

    eu

    Ti

    0 4 8 120

    0.2 W

    Mo

    24

    SUMMARY

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    Phase diagrams are useful tools to determine:

    --the number and types of phases,

    --the wt% of each phase,--and the composition of each phase

    for a given T and composition of the system.

    Chapter 9-25

    Alloying to produce a solid solution usually

    --increases the tensile strength (TS)

    --decreases the ductility.

    Binary eutectics and binary eutectoids allow for

    a range of microstructures.