Chapter 13 Thermo 2

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Transcript of Chapter 13 Thermo 2

  • Chemical Reaction Equilibria Chapter 13

    The Reaction CoordinateApplication of Equilibrium Criteria to Chemical ReactionsThe Standard G and the Equilibrium ConstantEffect on Temperature on the Equilibrium ConstantEvaluation of the Equilibrium ConstantRelation of Equilibrium Constant to CompositionEquilibrium Conversion for Single Reactions

  • Chemical Engineering Thermodynamics II ChE 342 12-2

    Introduction

    Transformation of raw materials into products having commercial use and value is a major industry.

    Raw Materials

    Products{crude oil, minerals, etc..} {Gasoline, NaOH, H2

    SO4

    , ammonia, etc..}

    This often involves chemical reactions and subsequent separation of the products.

    The rate and maximum (or equilibrium) conversion of chemical reaction are of important concern in its commercial development. Both of these aspects depend on the T, P, and composition of the reactants.

    We can often increase reaction rates by the use of CATALYST, but we can not change the equilibrium (or ultimate) conversion by using catalyst.

    D

    e

    g

    r

    e

    e

    o

    f

    r

    e

    a

    c

    t

    i

    o

    n

    Time

    With catalyst

    Withou

    t cataly

    st

    Uultimateconversion

  • Chemical Engineering Thermodynamics II ChE 342 12-3

    Chemical Reaction Course concerns on study of reaction rate and

    equilibrium, where the following tasks are often considered:

    Design and operation of reaction equipment Effect of controllable variables upon conversion Extent of reaction as t

    In general:Reaction Equilibrium is governed by THERMODYNAMICS

    while,Reaction Rate is governed by REACTION KINETICS

    Objectives:

    Definitions of reaction stoichiometry

    and criterion of reaction equilibrium. Dependence of equilibrium constant

    on temperature and its evaluation.

    Development of connection between equilibrium constant and composition.

    Calculation of equilibrium conversion

    for single reactions.

  • Chemical Engineering Thermodynamics II ChE 342 12-4

    The Reaction CoordinateThe general chemical reaction can be written as:

    44332211 +........++ AAAAwhere |i

    | are stoichiometric

    coefficients and Ai

    denotes the chemical formulas of species. i

    themselves are stoichiometric

    numbers

    Sign ConventionFor products: i

    is positive (+) For reactants: i

    is negative (-)

    N.B. The reaction, as written above, does not represent any mechanisms. It represents only the overall macroscopic picture. It does not tell us what is happening at the microscopic level. Example:

    CH4

    + H2

    O

    CO + 3H2CH4

    = -1CO

    = +1 H2

    = +3

    H2O

    = -1

    The stoichiomertric

    number of an inert species

    is zero.

    (I)

  • Chemical Engineering Thermodynamics II ChE 342 12-5

    In all reactions, the change in the number of moles of the species present are related to each other through the stoichiometric

    number.

    For example, for the reaction CH4

    + H2

    O

    CO + 3H2

    , if 0.5 mole CH4

    reacts, then 1.5 moles H2

    and 0.5 mol CO generated, thats ratio of change in number of moles to the stoichiometric

    number of CH4

    is the same as that for H2

    .Thus, in general for reaction (I), we can write:

    1

    1

    2

    2

    =

    dndn

    1

    1

    3

    3

    =

    dndn, , etc

    or, in general:

    .........=

    =

    = 3

    3

    2

    2

    1

    1 dndndn

    where d = the amount of reaction.d=

    It will be observed that the sign of i

    allows for the fact that:dni

    > 0 for the product & dni

    < 0 for the reactants The preceding equation provides the definition for , the Reaction Coordinate; a quantity characterizes the extent, or degree, to which chemical reaction has taken place.

    is also called the Degree of Reaction

    (II)

  • Chemical Engineering Thermodynamics II ChE 342 12-6

    From II, we can write,ddn ii =

    moles molesdimensionless

    By convention,

    = 0 at the initial state (before the reaction occurs). Integration yields:

    0

    =0

    i

    n

    ni ddn

    i

    i

    = f(t)

    nn iii += 0Summing over all N species (reactant and products) yields: +==

    0 iii nnnor, nn += 0 where, 0=0 inn = i&

    The quantity

    tells us whether there is a net increase or decrease in the total number of moles in the system. The mole fraction of species i

    at any time, or stage of reaction, is by:

    nn

    y ii = nn ii

    ++

    =0

    0This expression is very useful, since it provides us with a relationship between species concentration and the progress of the reaction.

    (III)

  • Chemical Engineering Thermodynamics II ChE 342 12-7

    Example:

    yCO 2+8+1

    =

    Consider the chemical reaction, CH4

    + H2

    O

    CO + 3H2Initially there present 2 moles CH4

    , 1 mole H2

    O, 1 mole CO and 4 moles H2

    . Obtain yi

    = f(). = i

    = -1 -1

    + 1 + 3 = 2 n0

    = n0i

    = 2 + 1 + 1 + 4 = 8 moles

    Application of the equation:

    yCH 28-2

    4 +=

    nn

    y iii ++

    =0

    0

    y OH 28-1

    2 +=

    yH 2834

    2 ++

    =

    Definition of a Mole of Reaction

    This means that

    has changed by a unit amount (i.e. 1 mol).

    When

    = 1 mole, the reaction proceeds to such an extent that the change in mole numbers for each reactant and product species is equal to its stoichiometric

    numbers, thats: ni = i

  • Chemical Engineering Thermodynamics II ChE 342 12-8

    Multireaction Stoichiometry

    In this case, we allocate a reaction coordinate, j

    , to each reaction

    (j

    = 1, 2, 3, R), where R

    = number of separate reactions.

    The stoichiometric

    numbers are now identified as:

    i,j Stoichiometric

    number of species i

    in reaction j

    ni

    may change because of the involvement of species i

    in several reactions. The general equation analogous to Eq. (III) for single reactions is:

    ,=j

    jjii ddn (i

    = 1, 2, .N;

    j = 1, 2, . , R)

    Integration yields; )(+= ,0j

    jjiii nn

    Summing over all species: )(+== ,0i j

    jjii nnn )(+= ,0j i

    jji n

    Similarly, ,=i

    jij v )(+= 0j

    jjnn

    Mole fraction,nn

    y ii =

    +

    )(+=

    0

    ,0

    jjj

    jjjii

    n

    n(i

    = 1, 2, . , N)

  • Chemical Engineering Thermodynamics II ChE 342 12-9

    Example: Consider the following reactions,CH4

    + H2

    O

    CO + 3H2 (1) j

    = 1CH4

    + 2H2

    O

    CO2

    + 4H2 (2) j

    = 2

    There are present 2 mol CH4

    and 3 mol H2

    O. Obtain expressions for yi

    = f(1

    , 2

    ).

    Construct the following table for i,j

    :

    i

    = CH4

    H2

    O CO CO2

    H2j

    12

    -1-1

    -1-2

    10

    01

    34

    j1

    = 22

    = 2

    )(+= 0j

    jjnn = 5 + 21

    + 22

    21

    21

    225--2

    4

    yCH ++=

    21

    21

    2252--3

    2

    y OH ++=

    21

    1

    2+2+5=

    yCO

    21

    2

    2+2+5=

    2

    yCO21

    21

    2+2+54+3

    =2

    yH

  • Chemical Engineering Thermodynamics II ChE 342 12-10

    Application of Equilibrium Criterion to Chemical ReactionsAs noted previously, in a closed system at equilibrium (constant

    T

    &P):

    (dGt)T,P

    = 0

    Recalling that Gt

    decreases during an irreversible process (eg. Mixing process, chemical rxn, etc) If a mixture is not in equilibrium, any reaction that occurs at

    constant T

    and P

    must

    lead to a decrease in the total energy of the system

    is the single variable that characterizes the progress of the reaction.

    Recall that

    is related to the composition of the system

    Criterion for equilibrium:1. (dGt)T,P

    = 02. Gt()

    is minimim

    N.B. Equilibrium expression can also be used for OPEN SYSTEM at constant T

    & P.

  • Chemical Engineering Thermodynamics II ChE 342 12-11

    The Standard Gibbs Energy Change and the Equilibrium Constant

    Recall the fundamental property relation for single-phase system:

    )(-)()(i

    iidndTnSdPnVnGd +=

    ddn ii =If changes in ni

    occur as a result of single reaction in a closed system, then:

    )(-)()(i

    ii ddTnSdPnVnGd +=

    =]

    )([ , iiPT

    nG= 0.0 At equilibrium state, according to the

    previous figure. The criterion for chemical reaction equilibrium can be expressed as:

    0.0= iiSince ii G =Recall that

    ln+)(= iii fRTT

    Write this equation for pure species in its standard state at the same temperature

    (A)

    oii

    oi fRTTG ln+)(= (B)

  • Chemical Engineering Thermodynamics II ChE 342 12-12

    See section 4.3 (p. 133) for the definition of standard state:Gases: pure species in ideal gas state at 1 bar (or 1 atm)Liquids or solids: actual pure liquid or solid at 1 bar (or 1 atm)

    Subtracting (B) from (A):o

    iioii ffRTG /ln=_

    ln= iaRTwhere is the activity of species i

    in solution.ia

    N.B. the activity coefficientia )/=(

    iiii fxfln+= i

    oii aRTGNow, & 0.0= ii

    0=]ln+[ 0 iiii aRTG 0=)ln(+][ 0 i

    iii aRTGor

    RTG

    a iivi i 0 -)(ln =or where product over all species

    ]/Exp[-)( 0 RTGa iivi i = = KGoi

    = f(T) only, independent of pressure; K

    = the equilibrium constant

    = f(T) only

    ln- ooii GGKRT == where G o

    the Standard Gibbs Energy Change of Reaction.

  • Chemical Engineering Thermodynamics II ChE 342 12-13

    Note: For a specific species the standard state represented by Gio

    must be the same state represented by fio

    upon which the activity coefficient is specified

    iaCase of Gases

    The standard state is the ideal gas state of pure species at a

    pressure of 1 bar. fio

    = 1 bar for each species in has phase reaction

    = =

    iii o

    i

    fa f

    f = ( ) i viK f must be measured in bar

    + for product, -

    for reactant

    Example: A + 2B + 3C

    D + 4 E

    -2 -3-1 4= ( ) = ( ) ( ) ( ) ( ) ( )i vi A B C D EK f f f f f for

    4

    2 3

    ( ) ( )=

    ( ) ( ) ( )

    D E

    A B C

    f fK

    f f fCase of liquids and solids

    The usual standard state is pure liquid or pure solid at 1 bar and T

    of the system. for this state, fio

    is not generally equal to 1 bar, thus =

    ii o

    i

    fa

    f

  • Chemical Engineering Thermodynamics II ChE 342 12-14

    Other Standard Property Change of ReactionFor the general property, M, we can write

    Mo

    = i

    Mio

    For example: Ho

    = i

    Hio

    CPo

    = i

    CPiof(T) only

    Relationship between Hio and GioPreviously, we have derived:

    Therefore, in the standard state for species i:

    = PT

    RTGT

    RTH

    ])/(

    - [

    =dT

    RTGdRTH

    oio

    i)/(

    - 2 = f(T)Why we removed the partial derivative?

    Summing over all species:

    = ][- 2

    RTG

    dTd

    RTHoiio

    ii

  • Chemical Engineering Thermodynamics II ChE 342 12-15

    = ][- 2RT

    GdTd

    RTHo

    o Relationship between Ho

    and Go

    But, RTGK o /-ln = 2lnRT

    HdT

    Kd o= Highly important

    relation

    Note: If Ho

    is negative (exothermic reactions) K

    as T

    Special case: Assuming Ho

    is independent of T,

    ]1

    -1

    [

    -)/ln(1

    1 TTRH

    KKo

    = A plot of lnK

    vs. 1/T

    should be a straight line

    See the next slide for plot of K

    versus 1/T

    for several reactions.

  • Chemical Engineering Thermodynamics II ChE 342 12-16

    This figure allows determination of K at any temperature.

    If K1

    is known at T1

    K

    can be determined at any temperature for a given Ho.

    Important Remarks:

    Slope of the lines are ve

    or +ve; -ve

    for endothermic reactions

    +ve

    for exothermic reactions

  • Chemical Engineering Thermodynamics II ChE 342 12-17

    Determination of Go

    K

    can be determined from the previous figure at a given temperature for certain

    reactions if Ho

    is constant (

    f(T)) Another alternative method, when Ho

    = f(T),

    for determination of K

    is by using:

    RTG

    Ko

    - ln = = f(T)

    If an estimate of Go

    is available K

    can be determined Recall that Go

    = f(T)

    Go

    can be calculated by using the general relation: ooo STHG - =

    Go

    = i

    GioHo

    = i

    HioSo

    = i

    SioCPo/R = i

    GPio/RRecalling (from Chapter 4 and 5):

    0

    0

    T

    T

    oPoo dT

    RC

    RHH += or: 0

    0

    T

    T

    oPoo

    TdT

    RC

    RSS +=

    Where H0o

    and S0o is the standard enthalpy and entropy changes at a reference temperature T0

    , respectively.

    (A)

    Substituting in (A) gives:

  • Chemical Engineering Thermodynamics II ChE 342 12-18

    00

    - -

    00

    T

    T

    oPo

    T

    T

    oPoo

    TdT

    RC

    RTSTdTRC

    RHG +=

    0

    000

    -

    TGH

    Soo

    o =

    According to (A):

    00

    -)-( -

    000

    0

    T

    T

    oPoo

    T

    T

    oPoo

    TdT

    RC

    RTGHTT

    dTRC

    RHG +=whence:

    00

    - 1-

    0

    000T

    T

    oP

    T

    T

    oP

    oooo

    TdT

    RC

    dTRC

    TRTHG

    RTH

    RTG

    ++=

    Division by RT:

    CPio/R = f(T)

    presented in Tables C.1-C.3 (pp. 657/658) Go

    and Ho

    values are tabulated for many formation reactions at standard conditions

    Gof298

    and Gof298

    (G0o

    and H0o) for a number of chemical compounds are listed in Table C.4 (pp. 569/660)

    Go/RT

    can be determined after determining the two integrals in the above equations

    Hence, K can be determined

  • Chemical Engineering Thermodynamics II ChE 342 12-19

    Example: calculate the equilibrium constant for the vapor-phase hydration of ethylene at 145 & 320oC from data given in Appendix C

    C2

    H4

    (g) + H2

    O(g)

    C2

    H5

    OH(g)

    Data: SpeciesC2

    H4

    (g)H2O(g)C2

    H5

    OH(g)

    i-1-1+1

    Ho29852510-241818-235100

    Go29868460

    -228572-168490

    Ai1.4243.473.518

    Bi

    10314.3941.45

    20.001

    Ci

    105-

    4.392-----

    -

    6.002

    where Cpi

    /R = Ai

    + Bi

    T

    + Ci

    T2

    298,o298 oii HH = = (-1)(52510) + (-1)(-241818)+(1)(-235100) = -

    45792 J/mol

    298,o298 oiiGG = = (-1)(52510) + (-1)(-241818)+(1)(-235100) = -

    45792 J/mol2

    ,o )()()/(/ TBTBARCRC iiiiiio iPiP ++==

    = [(-1)(1.424) + (-1)(3.47) + (1)(3.518)] + [(-1)(14.39) + (-1)(1.45) + (1)(20.0)]10-3T+ [(-1)(-4.392) + (-1)(0.0) + (1)(-6.002)]

    10-5T2

    = -1.376 + 4.157

    10-3T -

    1.61

    10-6T2

  • Chemical Engineering Thermodynamics II ChE 342 12-20

    418

    298

    26-3-

    418

    298

    26-3-

    ]101.61-104.157-1.376[-

    ]101.61-104.157-1.376[418

    1)298)(314.8(

    457928378-)418)(314.8(

    45792-

    TdT

    T

    dTTRTG o

    +

    +++

    +=

    @ T

    = 145oC = 418 K:

    936.1

    =RTG o@ T

    = 145oC = 418 K:

    RTG

    Ko

    - ln = K

    = exp(-1.936) = 0.1443

    Similarly @ T = 320oC = 593 K K

    = 0.00294

    K

    with TExothermic rxn

  • Chemical Engineering Thermodynamics II ChE 342 12-21

    Relationship between Equilibrium Constant and Composition

    Gas-Phase ReactionsFor the gas phase reactions: ( where fio

    = Po

    = 1 bar)= =

    iii o

    i

    fa f

    f i

    )( iifK =

    ),,( ii yPTff =K

    = f(T) only

    Reflects nonideality

    of the equilibrium mixture

    But

    &This means that for a given T, the composition at eqm

    must change

    with P

    in such away that remains constant iif )(

    Now, Pyf iii = i

    )( iii PyK =

    Separate P

    term, i ][)( ii PyK i= where = i

    Or, i- )( iii

    yPK =(recalling that yi

    can be related to e

    ) Relates K

    to e

    for a given T

    and P

    Complicated problem because: ),,( ii yPTf = iterative solution is needed

  • Chemical Engineering Thermodynamics II ChE 342 12-22

    Special cases: For equilibrium mixture as an ideal solution ii =

    whence, i- )( iii yPK =

    For sufficiently low pressure, equilibrium mixture behaves as an ideal gas

    1 =i

    whence, i- )( ii yPK = T, P, and composition-dependent terms are distinct are separate, thus solution for any one of

    e

    , T

    or P

    given the other two is straightforward Conclusion remarks

    -

    Dependence of T

    can be seen through K: If Ho

    +ve, ENDO

    rxn, K

    with T

    (yi

    )i

    for a fixed P

    e

    rxn

    shifts to the right

    If Ho

    -ve, EXO

    rxn, K

    with T

    (yi

    )i

    for a fixed P

    e

    rxn

    shifts to the left

    P

    @ constant T

    (yi

    )i

    rxn

    shifts to the right, e

    If

    (i

    ) -ve,-

    P

    @ constant T

    (yi

    )i

    rxn

    shifts to the left, e

    If

    (i

    ) +ve,

  • Chemical Engineering Thermodynamics II ChE 342 12-23

    Example: Consider the water-gas shift reactionCO(g) + H2

    O(g)

    CO2

    (g) + H2

    (g)Assuming ideal gas mixture, what is the fraction of the steam reacted in each of the following cases: (Hint: fraction of steam converted = (ni0

    nie

    )/ni0

    = -i

    e

    /ni0

    )(a) n0,H2O

    = 1, n0, CO

    = 1 mol, T

    = 1100 K, P

    = 1 bar

    n0

    = 2 mol & = 0.0From Fig. 13.2: @ 1/T

    = 1/(1100 K) = 9.09

    10-4

    for the above rxn

    lnK

    = 0 or K

    = 1.0

    1 = i i0 )( )1( iiyK = = 1

    14/)-1(4 2

    2

    =e

    e

    ,202

    02

    eeCO

    y =

    ++

    = ,2-1

    yCO = ,22e

    H

    y =2-1

    2

    y OH =

    Substituting:

    1y

    2

    2CO =OHCO

    H

    yyy

    e

    = 0.5 fraction of steam reacts = 0.5

    (b) n0,H2O

    = n0, CO

    = 1 mol, T

    = 1100 K, P

    = 10 bar Since

    = 0 P

    has no effect; e

    = 0.5

    (c) n0,H2O

    = n0, CO

    = 1 mol, n0,N2

    = 2 mol, T

    = 1100 K, P

    = 1 bar

    As an inert N2

    = 0 Does not affect the calculations, e

    remains the same.

  • Chemical Engineering Thermodynamics II ChE 342 12-24

    (d) n0,H2O

    = 2, n0, CO

    = 1 mol, T

    = 1100 K, P

    = 1 bar

    n0

    = 3 mol

    1)-1)(-2(

    2

    =ee

    e

    ,32e

    CO

    y = ,3-1

    yCO = ,32e

    H

    y =3-1

    2

    y OH =

    Substituting: e

    = 0.667 fraction of steam reacts = 0.667/2 = 0.33

    (e) n0,H2O

    = 1, n0, CO

    = 2 mol, T

    = 1100 K, P

    = 1 bar

    n0

    = 3 mol

    1)-1)(-2(

    2

    =ee

    e

    ,22e

    CO

    y = ,3-2

    yCO = ,32e

    H

    y =3-1

    2

    y OH =

    Substituting: e

    = 0.667 fraction of steam reacts = 0.667

    (f) n0,H2O

    = 2, n0, CO

    = 1 mol, n0, CO2

    = 1 mol, T

    = 1100 K, P

    = 1 bar

    n0

    = 3 mol

    1)-1(

    )1(2 =

    +

    e

    ee

    ,

    31

    2

    eCO

    y

    += ,3

    -1 yCO = ,32

    eH

    y =

    3-1

    2

    y OH =

    Substituting: e

    = 0.0.33 fraction of steam reacts = 0.33(g) n0,H2O

    = 1, n0, CO

    = 1 mol, T

    = 1650 K, P

    = 1 bar From Fig. 13.2: @ 1/T

    = 1/(1650 K)

    lnK

    = -1.15 or K

    = 0.316

    316.0)-1( 2

    2

    =e

    e

    e

    = 0.36

  • Chemical Engineering Thermodynamics II ChE 342 12-25

    Liquid-Phase ReactionsFor the liquid phase reactions: o

    i

    ii f

    fa

    = where fi

    o

    0

    iviaK )(

    =Then K

    remains as

    For liquid: iiii fxf =

    oi

    iiio

    i

    ii f

    fx

    ff

    a ==

    Determination of fi

    /fio:

    @ T

    and P: iii fRTTG ln)( +=@ T

    and Po: oii

    oi fRTTG ln)( +=

    Subtracting:

    Integration at constant T

    from Po

    to P:

    oii

    oii ffRTGG /ln- =

    But: dTSdPVdG ii i-=-P

    Pi

    oii

    odPVGG =

    (A)

    (B)

    Substitute (B) in (A): lnP

    Pio

    i

    i

    odPV

    ff

    RT =

    For liquids Vi

    is weak function of P

    upon integration )-(ln oioi

    i PPVff

    RT =

    or ]/)-(exp[ RTPPVff o

    ioi

    i =

  • Chemical Engineering Thermodynamics II ChE 342 12-26

    ]/)-(exp[ RTPPVxa oiiii =

    ioiii RTPPVxK }]/)-(exp{[=and

    io

    ii RT

    PPVii ex ][)(

    )-(=

    RTPPV

    ii

    oii

    i ex)-(

    )(=

    ])-(

    exp[])([ i

    ii

    oi

    ii VRTPPV

    xK i=

    Special cases At low P: exp[{Vi

    (P-Po)/RT}{i

    Vi

    }]

    1.0 (or when P

    Po)i

    iiixK )(= Requires determination i

    , but i

    = f(xi

    ) xi

    can be found in this case iteratively.

    For the case of ideal solution: i

    = 1.0

    iii

    xK )(= Law of Mass Action

    xi

    = f(e

    )

  • Chemical Engineering Thermodynamics II ChE 342 12-27

    Example: Esterification

    of acetic acid in the liquid phase at 100oC and 1 atm:

    CH3

    COOH(l) + C2

    H5

    OH(l)

    CH3

    COOC2

    H5

    (l) + H2

    O(l)

    Species

    i

    CH3

    COOH(l), i=1C2

    H5

    OH(l), i=2CH3

    COOC2

    H5

    (l), i=3H2

    O(l), i=4

    i-1-1+1+1

    Hof298 (J)-484,500-277690-480,000-285,830

    Gof298 (J)-389,900-174,780-332,200-273,129

    n0,acetic acid

    = n0,C2H5OH

    = 1 molEstimate the mole fraction of ethyl acetate (x3

    ) at equilibrium. Assuming ideal solution and that Ho

    does not change significantly with from 25oC to 100oC. i

    iixK )(=

    First, determine K: 298,o298 oii HH = = 484,500 + 277,690

    480,00

    285,830 = -

    3640 J

    298,o298 oiiGG = = 389,990 + 174,780 -332,200

    273,129 = -

    4650 J

    lnK

    = -Go/RT K298

    = exp[-4650/(8.314)(298)] K298

    = 6.527

  • Chemical Engineering Thermodynamics II ChE 342 12-28

    For constant Ho, apply the following,]

    1-

    1[

    -)/ln(

    11 TTR

    HKK

    o

    = ]2981

    -373

    1[

    314.83640

    -)527.6/ln( 373 =K

    K373

    = 4.859

    21

    34

    xxxx

    K =Now:

    K

    = 4.859, n0

    = 2, = 0

    0

    0

    nn

    x eiii+

    = ,2-1

    1ex = ,23

    ex = ,24ex =,

    2-1

    2ex =

    859.44/)-1(

    4/2

    2

    =e

    e

    e

    = 0.6879

    x3

    = 0.344

    (see other examples in the textbook)

    Chemical Reaction EquilibriaChapter 13IntroductionSlide Number 3The Reaction CoordinateSlide Number 5Slide Number 6Example:Multireaction StoichiometryExample:Application of Equilibrium Criterion to Chemical ReactionsThe Standard Gibbs Energy Change and the Equilibrium ConstantSlide Number 12Slide Number 13Other Standard Property Change of ReactionSlide Number 15Slide Number 16Determination of GoSlide Number 18Slide Number 19Slide Number 20Relationship between Equilibrium Constant and CompositionSlide Number 22Slide Number 23Slide Number 24Slide Number 25Slide Number 26Slide Number 27Slide Number 28