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    Lecture 4: Phase Equilibrium in Flowing Systems1

    Lecture 4: Phase Equilibrium in Flowing Systems

    In this lecture well show:

    How to apply thermodynamics to flowing systems

    Energy and entropy balances in flowing systems

    Availability and lost work

    Gibbs Phase Rule for flowing systems and system specification

    How data of mixture compositions are sometimes tabulated graphically.

    Graphical determination of vapor-liquid equilibrium of hydrocarbon systems

    Last lecture primarily focused on the thermodynamics of separations.

    We covered:

    Phase Stability and the Gibbs phase rule.

    A simple separation based on a vapor-liquid phase diagram.

    The lever rule.

    Equilibrium ratios (K-values, distribution coefficients, etc.).

    The activity, and activity coefficients.

    Measures of separations.

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    Lecture 4: Phase Equilibrium in Flowing Systems2

    Separation System Flows

    Streams in

    We can use the tools of entropy, energy, availability and mass balances to analyze

    any separations system:

    ...

    ...

    ...

    ...

    Streams out

    Heat in and heat out

    Work in and work out

    n, zi, T, P, h, s, b, v

    For each stream:

    n: molar flow rate

    zi: composition variables

    T: temperature

    P: pressure

    h: enthalpy

    s: entropy

    b: availability

    v: specific volume

    (ws)in (ws)out

    Qin Qout

    n, zi, T, P, h, s, b, v

    T0

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    Lecture 4: Phase Equilibrium in Flowing Systems3

    Balances and Availability

    Energy balance: nh Q Ws out

    nh Q Ws in

    0

    Entropy balance: ns Q

    Ts

    out

    ns Q

    Ts

    in

    Sirr

    Availability balance: nb Q 1T0Ts

    Ws

    in

    nb Q 1T0Ts

    Ws

    out

    LW

    b h T0sAvailability:

    Availability balance: Combine entropy balance, and energy balance

    with the definitions for lost work and availability.

    Lost work: LW T0Sirr

    Minimum work: nb

    out

    nbin

    WminThe minimum workfor a separation is

    the change in availability carried by the

    feed and product streams.

    Availability: the energy available in the system

    for conversion to shaft work.

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    Lecture 4: Phase Equilibrium in Flowing Systems4

    Gibbs Phase Rule

    F C 2

    The number of thermodynamic conditions that can be specified for a system with C components

    with phases in equilibrium.

    Variables: Equations:

    P

    T

    C (composition of each phase) C(-1)

    C +2 C(-1) +

    Xii

    1

    ki,

    Xi

    Xi

    Note that the Gibbs phase rule does not deal

    with flow variables or extensive variables.

    K-values are equations

    determined by

    thermodynamic

    equilibrium

    To extend the Gibbs Phase Rule to flow systems requiresAdding: Feed stream and extensive variables

    Adding: Independent equations relating variables

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    Lecture 4: Phase Equilibrium in Flowing Systems5

    Gibbs Phase Rule

    F C 2

    The number of thermodynamic conditions that can be specified for a system with 3 components

    with 3 phases in equilibrium.

    Variables: Equations:

    T, P,

    X1, X2, X3Y1, Y2, Y3Z1, Z2, Z3

    Xii

    1

    Yii

    1

    Zii

    1

    k1v,L

    Y1v

    Z1L

    k2v,L Y2

    v

    Z2L

    k3v,L

    Y3v

    Z3L

    k1v,S

    Y1v

    X1S

    k2v,S Y2

    v

    X2S

    k3v,S

    Y3v

    X3S

    Mole Fractions Equilibrium Conditions

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    Lecture 4: Phase Equilibrium in Flowing Systems6

    Gibbs Phase Rule for a Flowing System

    The number of thermodynamic conditions that can be specified for a system with 3 components

    with 3 phases in equilibrium.

    Variables: Equations:

    T, P,

    X1, X2, X3 ...Y1, Y2, Y3 ...

    Z1, Z2, Z3 ...

    Xii

    1

    Yii

    1

    Zii

    1} C

    F, Zi , TF , PF

    V, L, ...

    Q

    }

    C

    C 4

    C 2

    Additional

    Original

    ki, Xi

    Xi C 1

    Fzi Vyi Lxi ... C

    Fhf Q Vhv Lhl ... 1

    C C

    C1

    F C 2

    F 3

    F C 5For a flow system:

    Original

    Additional

    }

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    Determination of Unspecified Variables

    F, T, P, TF , PF , ZiF C 5If variables are used to specify

    Then remaining C 1 1 variables must be found from

    A) mole fraction summations

    B) K-Value relationships

    C) Mass balances

    D) Energy balance

    1 CC

    1

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    8/13Lecture 4: Phase Equilibrium in Flowing Systems8

    DePriester

    In order to carry out an analysis of a separation which uses differences in

    K-values between two phases to cause a separation, we need a source of

    K-values.

    A lot of equilibrium (K-Value) information forbinary systems is

    often contained in vapor-liquid phase diagrams.

    Forhydrocarbon systems, interactions between molecules are very similar,

    and consequently, the K-Values will not be a function of composition. K-Values

    at different pressures and temperatures for hydrocarbons can thus be graphed

    for multicomponent systems.

    One type of these graphs is called DePriester charts.

    Another type showing vapor-liquid equilibria for a multicomponent hydrocarbon

    system is shown in Figure 2.8 of the text.

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    DePriester Charts: Low T

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    DePriester Charts: High T

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    DePriester Charts: High T

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    DePriester

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    Summary

    In this lecture we discussed:

    How to carry out energy and entropy balances in flowing systems Availability and lost work

    Gibbs Phase Rule for flowing systems and system specification

    How to use DePriester charts to determine k-values for hydrocarbon vapor-liquid systems

    F C 5

    Next Lecture will focus on:

    Isothermal Flash calculations

    Derivation of the Rachford-Rice Equations

    Use of Newtons Iterative method to solve the RR equations

    An example using the RR procedure with Newtons method

    and DePriester charts to describe equilibrium