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    PENG ROBINSONEOS

    TEAM:

    -Marianella LucesIzarra

    -Soath Karime Parra

    -Javier Zozaya Pineda

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    Introduction The Peng-Robinson (PR) has become the most popular equation

    of state for natural gas systems in the petroleum industry.

    Place and date of discovery: during the decade of the 1970s,D.Peng was a PhD student of Prof. D.B. Robinson at the Universityof Calgary (Canada). In 1976 they developed The Peng andRobinson (PR) EOS, specifically focused on natural gas systems.

    Mean contribution: initially was found to calculate the volume of

    100% methane gas as a function of pressure and temperature.This equation expresses fluid properties in terms of the criticalproperties and acentric factor of each species involved.Nowadays it is applied to the representation of properties ofmixtures as well.

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    Preceding Correlations Van der Waals (1873):

    Is the simplest EOS and this equation is capable to describe the

    continuity between the liquid phase and vapor phase, to use it onlyneeds the knowledge of Tc and Pc, which are used to calculate theconstants a and b, as show the following equations:

    Where:

    a = Attraction parameter and b = Repulsion Parameter

    2v

    a

    bv

    TR

    P

    C

    C

    P

    TRa

    22

    421875,0

    c

    c

    P

    TRb

    125,0

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    Preceding Correlations Redlich and Kwong(RK) (1949) :

    RK modified the term of force attractionfrom the Van der Waals equation

    for a term dependent on the temperature:

    5,0)( Tbvv

    a

    bv

    TRP

    c

    c

    P

    TRa

    5,22

    42747,0

    c

    c

    P

    TR

    b

    08664,0

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    Preceding Correlations SoaveRedlichKwong (SRK) (1972) :

    SRK replaced the term dependent on the temperature of the equation of

    RK by an expression (T,

    )function of the temperature and of theacentric factor:

    )(

    )(

    bvv

    Ta

    bv

    TR

    P

    c

    cc

    P

    TR

    a

    22

    42747,0

    c

    c

    P

    TRb

    08664,0

    )()( TaaTa cc

    25,0

    11

    cT

    TkT

    2176,0574,1480,0 wwk

    = is the acentric factor

    of each pure substance ,

    this parameter measures

    the sphericity of the

    molecules

    k = is a constant

    characteristic of each

    substance

    (T) = dimensionless

    parameter dependently

    of T.

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    Equation Studied Peng and Robinson (PR) (1976):

    PR improved the prediction of Lparticularly closed to the criticalregion, treating the dimensionless factor for the attraction

    parameter as a function of acentric factor and reduced

    temperature:

    bvbbvva

    bv

    TRP

    )(

    c

    c

    P

    TR

    a

    22

    45724,0

    25,0

    11

    cT

    TkT

    22699,0574,13746,0 wwk

    c

    c

    P

    RTb 07780,0

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    Deriving the Equation PR departed from the equation of state of SRK improving liquid

    density values and accuracy for vapor pressures and equilibrium

    ratios.

    Base equation of SRK:

    PR proposed the need for an improvement in the ability of the

    equation of the state to predict liquid densities, particularly close

    to the critical region, as illustrated the following equation

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    Deriving the EquationAs VdW showed to determine the values of the two constants a and b

    PR solved these derivatives regardless of the type of substance and set an

    universal gas compressibility factor Z= 0.307 , and the parameters a and b

    can be calculated in a traditional way using in the following equations:

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    Deriving the EquationImportant: At temperatures others than critical the values of a and b,

    can be calculated using:

    Where (Tr, )will

    be equal to 1 at

    critical temperature

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    Deriving the EquationPR used the fugacity of each of the phases to determine the balance

    conditions of each phase, through the equation:

    The fugacity in each phase was introduced to develop a thermodynamic

    equilibrium. The fugacity is a measure of the potential for transfer of the

    components between phases ,where the phase with the lower componentfugacity accepts the component from the phase with a higher component

    fugacity. Therefore, the condition of the thermodynamic equilibrium can be

    expressed mathematically using the Newtonsmethod by:

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    Deriving the EquationWith a convergence criterion of L - V 10 -4 kPa about two to fouriterations were required to obtain the value of at each temperature.

    For all substances examined by PR the relationship between and Tc canbe described by the following equation:

    Where k is a constant characteristic of each substance:

    and is the acentric factor of each pure substance

    )1(1 2121 rTk

    226992.054226.137464.0 k

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    Deriving the Equation Rearranging the PR Equation of State

    It can be expressed as a cubic equation, in a more practical form in terms

    of the compressibility factor and replacing the molar volume with ZRT/P,as following:

    Where:

    For pure components:

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    Deriving the EquationAnd for mixtures:

    This Form of the equations produces one or three real roots depending

    upon the number of phases in the system. In the two phases region the

    largest root is for the compressibility factor of de vapor, while the smallest

    positive root corresponds to the liquid.

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    Considerations Used The PR parameters are expressed in function of the critical properties and acentric

    factor ().

    The equation shows accuracy values for Z and L at critical conditions.

    The mixing rules did not have to use more than one binary interaction parameter,

    which must be independent of P, T and composition. The mixture parameters used are

    defined for the following mixing rules:

    Where ij is an emp ir ical ly determined binary interaction co eff icient characterizing the binary formed b y

    comp onent i and j .

    The equations had to be applicable to calculate all the properties of the fluids for

    natural gas processes .

    i j

    ijTTjiT

    TTT

    i j

    TjiT

    j

    jj

    ji

    jiij

    ij

    aayya

    aaija

    ayyabyb

    )1()(

    ))(1(

    2/1

    2/1

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    Modifications Nikos et al. in 1986 proposed a generalized correlation for

    generating the binary interaction coefficient, .The authors correlated

    these coefficients with system pressure, temperature, and theacentric factor

    Where i refers to the principal component, N2, CO2, or CH4, and j

    refers to the other hydrocarbon component of the binary.

    The acentric-factor-dependent coefficients K0 K1 and K2, are

    determined for each set of binaries.

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    Modifications PR-VT, Stryjek-Vera (1986) proposed an improvement in the

    reproduction of vapor pressures of a pure component by the PR EOS, by

    replacing the K term in the equation

    with the following expression:

    0.7 < Tr < 1

    Tr

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    ModificationsCOMPONENT K

    1

    Nitrogen

    Carbon dioxide

    Water

    Methane

    Ethane

    Propane

    Butane

    Pentane

    Hexane

    Heptane

    Octane

    Nonane

    Decane

    Undecane

    Dodecane

    Tridecane

    Tetradecane

    Pentadecane

    Hexadecane

    Heptadecane

    Octadecane

    0.01996

    0.04285

    0.06635

    0.00159

    0.02669

    0.03136

    0.03443

    0.03946

    0.05104

    0.04648

    0.04464

    0.04104

    0.04510

    0.02919

    0.05426

    0.04157

    0.02686

    0.01892

    0.02665

    0.04048

    0.08291

    For components with a reduced

    temperature greater than 0.7,

    the optimum values of K1 for

    compounds of industrial interest

    are tabulated below:

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    Modifications Ahmed (1991) To use the Peng-Robinson equation of state to predict

    the phase and volumetric behavior of mixtures, one must be able to

    provide the critical pressure, the critical temperature, and the acentric

    factor for each component in the mixture. But the procedure isinadequate for calculating the parameters a, b, and of the equation for

    the C7+ fraction.

    parameter D as defined by the ratio of the molecular weight to the specific

    gravity of the heptanes-plus fraction:

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    ModificationsFor parameters a and b of C7+, the following generalized correlation

    is proposed

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    Solutions of the Equation Cubic Equation Generalized:

    Schmidt and Wenzel (1980) demonstrated that all the cubic equations of

    state can be expressed as:

    Liquid

    Vapor

    Other

    22wbubvv

    a

    bv

    TR

    P

    EOS u w

    VdW 0 0

    RK 1 0

    SRK 1 0

    PR 2 -1

    Heyen 1-w f(w,b

    )

    Kubic f(w) u2/4

    Patel-Teja 1-w f(w)

    Schmidt

    -Wenzel

    1-w f(w)

    Yu-Lu f(w) u-3

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    Solutions of the Equation Algorithm of the Equation

    Input Values

    Composition (Xi,Yi)

    Temperature and Pressure of operations(T,P)

    Acentric factor()

    Critical Pressure and Critical Temperature (Tc,Pc)

    Constant of gas (R)

    Calculate the parameters , b and for each component in the system.

    Calculate the mixture parameters and bmfor the gas and liquid phase.

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    Solutions of the Equation Calculate the coefficients A and B for the gas and liquid phase.

    Solve cubic equation for the compressibility factor of the gas and liquidphase.

    Obtain the root of cubic equation with the coefficients A and B

    Obtained Z you can calculate Volume or density.

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    Application in the Oil

    Industry The Peng-Robinson EOS has become the most popular equation of

    state for natural gas systems in the petroleum industry.

    A slightly better performance around critical conditions makes thePR EOS somewhat better suited to gas/condensate systems.

    PR obtains better liquid densities than SRK.

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    Thank You!