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1 MSE 303 Thermodynamics & Equilibrium Processes Calculating Phase Diagrams
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MSE 303_Note8_Calculating Phase Diagrams (Gaskel Chap10).pdf

Nov 18, 2015

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MSE 303_Note8_Calculating Phase Diagrams (Gaskel Chap10).pdf
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  • MSE 303, Fall 2012 1

    MSE 303

    Thermodynamics & Equilibrium Processes

    Calculating Phase Diagrams

  • MSE 303, Fall 2012 2

  • MSE 303, Fall 2012 3

    Temperature, T1

    Calculate the Gibbs free energy G as a function of composition at T = T1 for liquid and solid phases

    Liquid has lower energy over entire composition range

    Hence at T1, our phase diagram must show liquid phase across entire composition

  • MSE 303, Fall 2012 4

    Temperature, T2

    This equivalence of Gibbs free energy indicates a phase transition from liquid to solid state

  • MSE 303, Fall 2012 5

    Temperature, T3

    This indicates that two phases: Liquid and solid are in equilibrium

  • MSE 303, Fall 2012 6

    Temperature, T4

  • MSE 303, Fall 2012 7

    Based on the free energy curves we have generated, we can now construct the phase diagram

    A B

    L

    S

    L

    L+S

    S S

    L

    L

    S All temperatures between T2 and T4 are have similar curve

  • MSE 303, Fall 2012 8

    Actual Example

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  • MSE 303, Fall 2012 10

    Binary Solution with Miscibility Gap

  • MSE 303, Fall 2012 11

    Binary Solution with Miscibility Gap

  • MSE 303, Fall 2012 12

    Eutectic Phase Diagram

  • MSE 303, Fall 2012 13

    Eutectic Phase Diagram

  • MSE 303, Fall 2012 14

    Gibbs Free Energy Curve vs Composition, GM(Xi)

    Partial molar Gibbs Free Energies of component in different phases

    The partial molar Gibbs free energy change due to introduction of component i into the solution

    General principles of calculating phase diagrams:

  • MSE 303, Fall 2012 15

    Gibbs Free Energy Curve vs Composition, GM(Xi)

    The curve relating Gibbs free energy to composition if solutions exhibit ideal behavior:

    To be able to calculate partial molar free energy of a component I (or A or B), It is convenient to choose a standard state at which we define Gi0 as zero

  • MSE 303, Fall 2012 16

    Gibbs Free Energy Curve vs Composition, GM(Xi)

  • MSE 303, Fall 2012 17

    Figure 10.2 The activities of component B obtained from lines I, II, and III in Fig. 10.1.

  • MSE 303, Fall 2012

    Figure 10.8 (a) The phase diagram for the system AB. (b) The Gibbs free energies of mixing in the system AB at the temperature T.

  • MSE 303, Fall 2012 19

    Check at XA =1, XA=0

  • MSE 303, Fall 2012 20

    Check at XB =1, XB=0

    liquid

    Similarly at The formation of an ideal solid solution from liquid A and solid B

  • MSE 303, Fall 2012 21

    At any composition the formation of a homogeneous liquid solution from pure liquid A and pure solid B can be considered as being a two-step process involving 1. The melting of XB moles of B, which involves the change in Gibbs free energy 2. The mixing of XB moles of liquid B and XA moles of liquid A to form an ideal liquid solution, which involves the change in Gibbs free energy,

  • MSE 303, Fall 2012 22

    ideal liquid solution from liquid A and solid B

    Similarly, at any composition, the formation of an ideal solid solution from liquid A and solid B involves a change in Gibbs free energy of

    ( l ) 10.5

    10.6

  • MSE 303, Fall 2012 23

    From (1)

    ( l )

    ( l )

    From chapter 9,

    10.7

    10.8

  • MSE 303, Fall 2012 24

    From 10.6,

    10.10

    (6)

    Also use

    We got

    10.9

  • MSE 303, Fall 2012 25

    Similarly,

    The solidus and liquidus compositions are thus determined as follows

  • MSE 303, Fall 2012 26

    Position of solidus and liquidus can be calculated at any temperature

  • MSE 303, Fall 2012 27

    assuming ideal solution behavior, we can calculate G0m and the phase diagram

  • MSE 303, Fall 2012 28

    Given

  • MSE 303, Fall 2012 29

  • MSE 303, Fall 2012 30

    Assuming ideal binary liquid and solid solutions

  • MSE 303, Fall 2012 31

  • MSE 303, Fall 2012 32

    In (a), liquid A and solid B are chosen as standard states located at G=0

    In (b), liquid A and liquid B are chosen as standard states located at G=0

    In (c), solid A and solid B are chosen as standard states located at G=0

    Fig. 10.10 shows the Gibbs free energy of mixing curves for a binary system AB which forms ideal solid solutions and ideal liquid solutions, drawn at a temperature of 500 K, which is lower than Tm,(B) and higher than Tm,(A). At and

  • MSE 303, Fall 2012 33

    Example 2: Gaskell page 287

    Consider a phase diagram that exhibits complete miscibility in the liquid state and complete immiscibility in the solid state

    At the indicated composition, at temperature T, we have pure A in equilibrium with the liquid solution having the composition of the point p

    p

    AlA

    AlsA

    aRTG

    GG

    ln0 )(

    )(0)(

    +=

    =

    Same as

    with aA=XA for Routian liquid

    Thus,

  • MSE 303, Fall 2012 34

    Consider using this equation to calculate the liquidus lines in a binary eutectic system Take for example, the Cd-Bi system

    If liquidus solutions are ideal, we can calculate the Bi liquidus from

  • MSE 303, Fall 2012 35

  • MSE 303, Fall 2012 36

    or

  • MSE 303, Fall 2012 37

  • MSE 303, Fall 2012 38

  • MSE 303, Fall 2012 39

  • MSE 303, Fall 2012 40