Page 228 - Characterization and Properties of Petroleum Fractions - M.R. Riazi
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            AT029-Manual
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                                           August 16, 2007
         208 CHARACTERIZATION AND PROPERTIES OF PETROLEUM FRACTIONS
         is weak. Usually the SRK equation predicts densities more ac-
         curately for compounds with low acentric values, while the  5.5.4 Other Types of Cubic Equations of State
         PR predicts better densities for compounds with acentric fac-  In 1972 Saove for the first time correlated parameter a in a
         tors near 0.33 [21]. For this reason a correction term, known  cubic EOS to both T r and ω as given in Table 5.1. Since then
         as volume translation, has been proposed for improving vol-  this approach has been used by many researchers who tried
         umetric prediction of these equations [8, 15, 19, 22]:  to improve performance of cubic equations. Many modifica-
                                                              tions have been made on the form of f ω for either SRK or
        (5.50)              V = V EOS  − c                    PR equations. Graboski and Daubert modified the constants
                                                              in the f ω relation for the SRK to improve prediction of va-
         where c is the volume translation parameter and has the same  por pressure of hydrocarbons [24]. Robinson and Peng [14]
         unit as the molar volume. Equation (5.50) can be applied to  also proposed a modification to their f ω equation given in
         both vapor and liquid volumes. Parameter c mainly improves  Table 5.1 to improve performance of their equation for heav-
         liquid volume predictions and it has no effect on vapor pres-  ier compounds. They suggested that for the PR EOS and for
         sure and VLE calculations. Its effect on vapor volume is negli-  compounds with ω> 0.49 the following relation should be
                   V
         gible since V is very large in comparison with c, but it greatly  used to calculate f ω :
         improves prediction of liquid phase molar volumes. Values of                          2          3
         c have been determined for a number of pure components up  (5.53)  f ω = 0.3796 + 1.485ω − 0.1644ω + 0.01667ω
         to C 10 for both SRK and PR equations and have been included  Some other modifications give different functions for param-
         in references in the petroleum industry [19]. Peneloux et al.  eter α in Eq. (5.41). For example, Twu et al. [25] developed
         [22] originally obtained values of c for some compounds for  the following relation for the PR equation.
         use with the SRK equation. They also suggested the following     −0.171813              1.77634
         correlation for estimation of c for SRK equation:           α = T r     exp 0.125283 1 − T r


                                                              (5.54)     + ω T −0.607352  exp 0.511614 1 − T 2.20517

                                            RT c                              r                      r
        (5.51)      c = 0.40768 (0.29441 − Z RA)                                −0.171813              1.77634
                                             P c                             − T r    exp 0.125283 1 − T r
         where Z RA is the Rackett parameter, which will be discussed  Other modifications of cubic equations have been derived by
         in Section 5.8.1. Similarly Jhaveri and Yougren [23] obtained  suggesting different integer values for parameters u 1 and u 2 in
         parameter c for a number of pure substances for use with PR  Eq. (5.40). One can imagine that by changing values of u 1 and
         EOS and for hydrocarbon systems have been correlated to  u 2 in Eq. (5.40) various forms of cubic equations can be ob-
         molecular weight for different families as follows:  tained. For example, most recently a modified two-parameter
                                                              cubic equation has been proposed by Moshfeghian that cor-
                      c P = b PR 1 − 2.258M P −0.1823         responds to u 1 = 2 and u 2 =−2 and considers both parame-

        (5.52)        c N = b PR 1 − 3.004M −0.2324           ters a and b as temperature-dependent [26]. Poling et al. [8]

                                       N

                      c A = b PR 1 − 2.516M −0.2008           have summarized more than two dozens types of cubic equa-
                                       A                      tions into a generalized equation similar to Eq. (5.42). Some
         where b PR refers to parameter b for the PR equation as given  of these modifications have been proposed for special sys-
         in Table 5.1. Subscripts P, N, and A refer to paraffinic, naph-  tems. However, for hydrocarbon systems the original forms
         thenic, and aromatic hydrocarbon groups. The ratio of c/b  of SRK and PR are still being used in the petroleum industry.
         is also called shift parameter. The following example shows  The most successful modification was proposed by Zudke-
         application of this method.                          vitch and Joffe [27] to improve volumetric prediction of RK
                                                              EOS without sacrificing VLE capabilities. They suggested that
                                                              parameter b in the RK EOS may be modified similar to Eq.
         Example 5.3—For the system of Example 5.2, estimate V L  (5.41) for parameter a as following:
              V
         and V for the PR EOS using the volume translation method.
                                                              (5.55)                b = b RK β
         Solution—For n-C 8 , from Table 2.1, M = 114 and b PR are  where β is a dimensionless correction factor for parameter
                                          3
         calculated from Table 5.1 as 147.73 cm /mol. Since the hy-  b and it is a function of temperature. Later Joffe et al. [28]
         drocarbon is paraffinic Eq. (5.51) for c P should be used,  determined parameter α in Eq. (5.41) and β in Eq. (5.55) by
                 3
         c = 7.1cm /mol. From Table 5.2, V L(PR)  = 356.2 and V V(PR)  =  matching saturated liquid density and vapor pressure data
                 3
         1196.2cm /mol. From Eq. (5.50) the corrected molar volumes  over a range of temperature for various pure compounds. In
             L
         are V = 356.2 − 7.1 = 349.1 and V = 1196.2 − 7.1 = 1189.1  this approach for every case parameters α and β should be
                                     V
         cm /mol. By the volume translation correction, error for V L  determined and a single dataset is not suitable for use in all
           3
         decreases from 17.2 to 14.8% while for V it has lesser effect  cases. SRK and ZJRK are perhaps the most widespread cu-
                                           V
         and it increases error from –1.6% to –2.2%.          bic equations being used in the petroleum industry, especially
                                                              for phase behavior studies of reservoir fluids [19]. Other re-
          As is seen in this example improvement of liquid volume  searchers have also tried to correlate parameters α and β in
         by volume translation method is limited. Moreover, estima-  Eqs. (5.41) and (5.55) with temperature. Feyzi et al. [29] cor-
         tion of c by Eq. (5.51) is limited to those compounds whose  related α 1/2  and β 1/2  for PR EOS in terms T r and ω for heavy
         Z RA is known. With this modification at least four parameters  reservoir fluids and near the critical region. Their correla-
         namely T c , P c , ω, and c must be known for a compound to  tions particularly improve liquid density prediction in com-
         determine its volumetric properties.                 parison with SRK and PR equations while it has similar VLE





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