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         52 CHARACTERIZATION AND PROPERTIES OF PETROLEUM FRACTIONS
                             Reduced Boiling Point, Tbr  T1: IML  August 16, 2007  16:6























                                                       Molecular Weight
                              FIG. 2.1—Reduced boiling point of homologous hydrocarbon groups from
                            Eq. (2.42).

         d ∞ = 0.8541 and n ∞ = 1.478 (I ∞ = 0.283), while the values  Pan et al. [63, 64] also recommend use of the following re-
         obtained through Eq. (2.42) (see Table 2.6) are T b∞ = 1070,  lation for the acentric factor of aromatics for hydrocarbons
         d ∞ = 0.859, and I ∞ = 0.2833. One can see how close the val-  with M < 800:
         ues are although they have been derived by two different                               0.026261            --`,```,`,``````,`,````,```,,-`-`,,`,,`,`,,`---
         methods. However, these values are of little practical applica-  (2.44)  ln ω =−36.1544 + 30.94M
         tion as long as a proposed correlation satisfies the condition  and when M > 800, ω = 2.0. Equation (2.42) is recommended
         of T br = 1at P c = 1.0133 bar. Equation (2.42) will be used later  for calculation of other thermodynamic properties based on
         in Chapter 4 to develop physical properties of single carbon  the evaluation made on thermodynamic properties of waxes
         number (SCN) cuts up to C 50 for the estimation of properties  and asphaltenes [63, 64].
         of heavy crude oils and reservoir oils. Graphical presentation  For homologous hydrocarbon groups, various correlations
         of Eq. (2.42) for T br and T c versus molecular weight of dif-  may be found suitable for the critical properties. For example,
         ferent hydrocarbon families is shown in Figs. 2.1 and 2.2 for  another relation that was found to be applicable to critical
         molecular weights up to 3000 (N C = 214).            pressure of n-alkyl families is in the following form:
                                     ∼
          One direct application of critical properties of homologous                       −n
         hydrocarbons is to calculate phase equilibrium calculations  (2.45)     P c = (a + bM)
         for wax precipitation and cloud point of reservoir fluids and  where P c is in bar and M is the molecular weight of pure hy-
         crude oils as shown by Pan et al. [63, 64]. These investigators  drocarbon from a homologous group. Constant n is greater
         evaluated properties calculated through Eq. (2.42) and mod-  than unity and as a result as M →∞ we have P c → 0, which
         ified this equation for the critical pressure of PNA hydrocar-  satisfies the general criteria for a P c correlation. Based on data
         bons with molecular weight above 300 through the following  on P c of n-alkanes from C 2 to C 22 , as given in Table 2.1, it was
         relation:                                            found that n = 1.25, a = 0.032688, and b = 0.000385, which
                                                                    2
                                                              gives R = 0.9995 with average deviation of 0.75% for 21 com-
        (2.43)           P c = a − b exp(−cM)
                                                              pounds. To show the degree of extrapolation of this equation,
         where a, b, and c are given for the three hydrocarbon groups  if data from C 2 to C 10 (only nine compounds) are used to
         in Table 2.8 [64]. However, Eq. (2.43) does not hold the inter-
         nal consistency at P c of 1 atm, which was imposed in deriving
         the constants of Eq. (2.42). But this may not affect results for  TABLE 2.8—Coefficients of Eq. (2.43).
         practical calculations as critical pressures of even the heaviest  Coefficient  Paraffins  Naphthenes  Aromatics
                                                                           0.679091
                                                                                          2.58854
                                                                                                        4.85196
         compounds do not reach to atmospheric pressure. A compar-  a b  −22.1796       −27.6292      −42.9311
         ison between Eq. (2.42) and (2.43) for the critical pressure  c   0.00284174     0.00449506    0.00561927
         of paraffins, naphthenes, and aromatics is shown in Fig. 2.3.  Taken from Pan et al. [63, 64].













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