Page 466 - Standard Handbook Petroleum Natural Gas Engineering VOLUME2
P. 466

444    Production


                  (ht continuad fsom page  419)
                  while the data from Table 6-20 was used for the Benedict-Webb-Rubin equation
                  modified by Starling [16].
                    Applying Peng-Robinson equation






                  or

                                                A             z + (za5 + 1)~
                     hei = - h(Z - B) + (Z - 1)BI - -(A;   - B;)          1     (6-536)
                                               2l.5 B         Z - (qas - l)B

                  where

                         bi
                     Bi  =-                                                      (6-54)
                         b

                                                                                 (6-55)


                  Notations are as in Equations 6-13 and 6-14.
                    The objectives of  any equation-of-state solution method are the reliable and
                  accurate prediction  of  the  volumetric properties  of  the  fluid  mixture under
                  consideration. The overall solution procedure is  as follows:
                      fix the total composition, temperature and pressure
                      calculate constants for the equation of  state
                      solve equation  for  the  volumetric property  (specific volume,  density or
                       compressibility factor)

                  When pressure and temperature fall to a two-phase region, the equation must
                  be solved twice, separately for vapor and liquid. The composition of  each phase
                  will be different so  the equation of state constants will have to be evaluated for
                  both  the liquid and the vapor phases. Both SRK and PR  are cubic equations,
                   so  the solution always gives three roots, as is shown in Figure 631 [17]. However,
                   the  Pr-Vr relationship at a  given T,  is  discontinuous at Vr = b;,  Vr = b;,  and
                  Vr = b;.  We  are interested in only Vr > b;,  which  in case the SRK  equation is
                   equal 0.08664 and 0.077796 for the PR equation. For Vr > b;  and T, > 1.0, there
                   is only one value of  the compressibility factor that will  satisfy the equation of
                   state. For  Vr > b;  and Tr < 1.0 we  will  get three values of  Z.  The largest Z  of
                   the vapor Z’s  is chosen for the vapor and the smallest amount the liquid Z’s is
                   chosen for the liquid. However,  in an earlier stage of  the iterative VLE calcula-
                   tions, it is not Uncommon to encounter a single root, mainly because of incorrect
                   compositions [17].
                    A logic diagram for a trial-and-error solution procedure for cubic equations
                   of  state is  given  in  Figure 6-32. This  diagram  shows a  traditional  Newton-
                   Raphson approach with an interval halving limiting procedure superimposed on
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