Page 390 - Characterization and Properties of Petroleum Fractions - M.R. Riazi
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P2: IML/FFX
                           QC: IML/FFX
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                        AT029-Manual-v7.cls
            AT029-Manual
  AT029-09
                                           June 22, 2007
         370 CHARACTERIZATION AND PROPERTIES OF PETROLEUM FRACTIONS
                             TABLE 9.2—Characterization parameters of the C 7+ fraction of sample of Table 9.1 [7].
                                                           SG
                      Pseudocomponent  mol% T1: IML  M  14:25    T b ,K  n 20   N C   P%    N%   A%
                                            wt%
                      C 7+ (1)       10.0   12.5   110    0.750  391.8  1.419    8    58    22   20
                      C 7+ (2)        9.0   17.1   168    0.810  487.9  1.450   12.3  32    35   33
                      C 7+ (3)        7.7   23.1   263    0.862  602.1  1.478   19.3  17    37   46
                      C 7+ (4)        2.5   11.6   402    0.903  709.0  1.501   28.9   6    34   60
                      C 7+ (5)        1.2    8.2   608    0.949  777.6  1.538   44     0    45   55
                                     30.4   72.5   209.8  0.843  576.7  1.469   15.3  25    34   41
                      Total C 7+
                      Experimental values on M 7+ and SG 7+ . Distribution parameters (for Eq. 4.56) and calculated values: M 7+ = 209.8; M o =
                      86.8; S o = 0.65; S 7+ = 0.844; B M = 1; A s = 0.119; n 7+ = 1.4698; A M = 1.417; B S = 3; M av = 209.8; S av = 0.847.
         characterization parameters (i.e., M, T b , SG, n 20 , N C , and PNA  ponent of heptane-plus, C 7 (1). The value of BIP of this pair
         composition). This is done using the distribution model de-  exhibits a major impact in the calculation results. K i values
         scribed in Section 4.5.4 with M 7+ and SG 7+ as the input pa-  are calculated from SRK EOS and flash calculations are per-
         rameters. The basic parameters (T b , n 20 ) are calculated from  formed for three stages shown in Fig. 9.3. The liquid product
             --`,```,`,``````,`,````,```,,-`-`,,`,,`,`,,`---
         the methods described in Chapter 2, while the PNA composi-  from the first stage is used as the feed for the second stage
         tion for each pseudocomponent is calculated from methods  separator and flash calculation for this stage is performed
         given in Section 3.5.1.2 (Eqs. 3.74–3.81). The calculation re-  to calculate composition of feed for the last stage. Similarly,
         sults with distribution parameters for Eq. (4.56) are given in  the final crude oil is produced from the third stage at atmo-
                                                              spheric pressure. Composition of C 7+ in each stream can be
         Table 9.2. Molar and specific gravity distributions of the C 7+
         fraction are shown in Fig. 9.4. The PNA composition is needed  calculated from sum of mole fractions of the five pseudocom-
         for calculation of properties through pseudocomponent ap-  ponents of C 7i . GOR for each stage is calculated from Eq. (9.8).
         proach (Section 3.3.4). Such information is also needed when  Summary of results are given in Table 9.3. Overall GOR is cal-
         a simulator (i.e., EOR software) is used for phase behavior  culated as 853 compared with actual value of 850 scf/stb. This
         calculations [9].                                    is a very good prediction mainly due to adjusting BIPs with
          To generate the composition of gases and liquids in sepa-  liquid density of produced crude oil. The calculated composi-
         rators, see Fig. 9.3, the feed to the first stage is considered  tions in Table 9.3 are also in good agreement with actual data
         as a mixture of 17 components (12 components listed in  of Table 9.1.
         Table 9.1 and 5 components listed in Table 9.2). For pure com-  The method of characterization selected for treatment of
         ponents (first 11 components of Table 9.1), T c , P c , V c , and ω are  C 7+ has a major impact on the results of calculations as shown
         taken from Table 2.1. For C 6 fraction (SCN) and C 7+ fractions  by Riazi et al. [7]. Table 9.4 shows results of GOR calcu-
         (Table 9.3) critical properties can be obtained from methods  lations for the three stages from different characterization
         of Chapter 2 (Section 2.5) or from Table 4.6. For this example,  methods. In the Standing method, Eqs. (6.204) and (6.205)
         Lee–Kesler correlations for calculation of T c , P c , and ω and  have been used to estimate K i values, assuming ideal solution
         Riazi–Daubert correlations (the API methods) for calculation  mixture. As shown in this table, as the number of pseudocom-
         of V c and M (or T b ) have been used. The binary interaction pa-  ponents for the C 7+ fraction increases better results can be
         rameters (BIPs) for nonhydrocarbon–hydrocarbon are taken  obtained.
         from Table 5.3 and for hydrocarbon–hydrocarbon pairs are
         calculated from Eq. (5.63). Parameter A in this equation has
         been used as an adjustable parameter so that at least one pre-  9.2.2 Bubble and Dew Points Calculations
         dicted property matches the experimental data. This property
         can be saturation pressure or a liquid density data. For this  Bubble point pressure calculation is performed through the
         calculation, parameter A was determined so that predicted  following steps:
         liquid specific gravity from last stage matches experimental
         value of 0.815. Liquid SG is calculated from Eq. (7.4) using  1. Assume a liquid mixture of known x i and T is available.
                                                                          sat
         SG of all components in the mixture. It was found that when  2. Calculate P i  (vapor pressure) of all components at T from
         A = 0.18, a good match is obtained. Another adjustable pa-  methods described in Section 7.3.
         rameter can be the BIP of methane and the first pseudocom-  3. Calculate initial values of y i and P bub from Raoult’s law as
                                                                         sat          sat
                                                                P =   x i P i  and y i = x i P i  P.
                                                              4. Calculate K i from Eq. (6.197) using T, P, x i , and y i .

             0.01                        4                    5. Check if      x i K i − 1 <ε, where ε is a convergence toler-


            0.008                                               ance, (e.g., 1 × 10 −12 ) and then go to Step 6. If not, repeat
                                         3
            0.006                                               calculations from Step 4 by guessing a new value for pres-
           F(M)  0.004                 F(SG)  2                 sure P and y i = K i x i .If     x i K i − 1 < 0, reduce P and if
                                                                   x i K i − 1 > 0, increase value of P.
            0.002                        1
                                                              6. Write P as the bubble point pressure and y i as the com-
               0                         0                      position of vapor phase. Bubble P can also be calculated
                0  200 400 600 800       0.6 0.8  1  1.2 1.4
                                                                through flash calculations by finding a pressure at which
                       M                         SG             V F = 0. In bubble T calculation x i and P are known. The
                                                                   ∼
           FIG. 9.4—Probability density functions for molecular  calculation procedure is similar to bubble P calculation
         weight and specific gravity of the C 7+ fraction given in  method except that T must be guessed instead of guess-
         Table 9.2 [8].                                         ing P.











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