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2.5  Nonideal Thermodynamic Property Models  43


         engineers  because  its  range  of  application  is  too  narrow.   corresponding  to  the  vapor  phase-that   is,  Zv-and   the
         However, its development did suggest that all species might   smallest Z (smallest v) corresponding to the liquid phase-
         have equal reduced molar volumes, v,  = vlv,,  at the same   that is, ZL. The intermediate value of Z is of no practical use.
         reduced  temperature,  x. = TIT,,  and  reduced  pressure,   To apply the R-K  equation to mixtures, mixing rules are
         p,  = PIP,.  This finding, referred to as the law (principle or   used to average the constants a and b for each component in
         theorem) of  corresponding states, was utilized to develop the   the mixture. The recommended rules for vapor mixtures of C
                  equation of state given as (2) in Table 2.5. That   components are
         equation  defines the  coinpressibility factol;  Z,  which  is  a
         function of P,, T,,  and the critical compressibility factor, Z,,
         or the acentric factol;  w,  which is determined from experi-
         mental P-V-T  data. The acentric factor, introduced by Pitzer
         et a]. [17], accounts for differences in molecular shape and is
         determined from the vapor pressure curve:


                                                            EXAMPLE 2.5
                                                            Glanville, Sage, and  Lacey  [20] measured  specific  volumes  of
         This definition results in a value for w of zero for symmetric
                                                            vapor  and  liquid  mixtures  of  propane  and  benzene  over  wide
                  Some typical values of w  are 0.264, 0.490, and   ranges of temperature and pressure. Use the R-K  equation to esti-
         0.649 for toluene, n-decane, and ethyl alcohol, respectively,   mate  specific volume of  a vapor mixture  containing 26.92 wt%
         as taken from the extensive tabulation of Poling et al. [ll].   propane at 400°F (477.6 K) and a saturation pressure of 410.3 psia
           In  1949, Redlich and Kwong [I81 published an equation   (2,829  kPa). Compare the estimated and experimental values.
         of state that, like the van der Waals equation, contains only
         two constants, both of which can be determined from T,  and
                                                            SOLUTION
         PC, by applying the critical conditions
                                                            Let propane be denoted by P and benzene by B. The mole fractions
                                      ($),                  are
                         0
                (g)Tc  and                    =  o
                       =
         However, the R-K  equation, given as (3) in Table 2.5, is a
         considerable improvement over the van der Waals equation.
         A study by  Shah and Thodos  [19] showed that the simple
         R-K  equation, when applied to nonpolar compounds, has an
                                                            The critical constants for propane and benzene are given by Poling
         accuracy that compares quite favorably with equations con-   et al. [ll]:
         taining many more constants. Furthermore, the R-K  equa-
         tion can approximate the liquid-phase region.
           If  the  R-K  equation  is  expanded  to  obtain  a  common          Propane       Benzene
        denominator,  a  cubic  equation  in  v  results.  Alternatively,
        (2) and (3) in Table 2.5 can be combined to eliminate v to
        give the compressibility factor, Z, form of the R-K  equation:

                                                            From the equations for the constants b and a in Table 2.5 for the
                                                            R-K  equation, using SI units,
        where









           Equation (2-46), which is cubic in Z, can be solved ana-
                                                           Similarly,
        lytically for three roots (e.g., see Perry's Handbook, 7th ed.,
                                                                          bB = 0.08263 m3/kmol
        P.  4-20).  In  general,  at  supercritical  temperatures,  where
        only one phase can exist, one real root and a complex conju-      a~ = 2,072 kPa-m6/kmo12
        gate pair of roots are obtained. Below the critical tempera-
                                                           From (2-50),
        ture, where vapor and/or  liquid phases can exist, three real
        roots  are obtained, with  the  largest  value  of  Z  (largest  v)
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