Page 444 - Standard Handbook Petroleum Natural Gas Engineering VOLUME2
P. 444

406    Production


                   (to assure that the mixture is in two-phase region) cannot be conveniently used
                   in most computer equation-of-state-based flash calculations because the K values
                   for  a  given  system are  not  known  until  the  final  solution has been  reached.
                   Consequently, the  flash  calculation  (and it  convergence algorithm) must  be
                   capable of  performing "flash calculation" on  single phase systems (subcooled
                   liquids, superheated vapors and dense gas systems) as well as reliably predicting
                   the amount of vapor and liquid present in a two-phase system. When the above
                   flash equation/convergence  algorithm is used on single phase systems, the final
                   predicted value of  L/F  will  usually be outside the interval described by  Equa-
                   tion 6-25 unless the material balance constraint is enforced. Should a value of
                   (L/F)"+'  outside the  limits defined by  Equation 6-25 be  detected in  an inter-
                   action, we  recommend that  the value of  L/F  predicted by  Equation 6-24a be
                   replaced by  the appropriate value described by  the following equations:
                     if  (L/F),+'  < 0.0,   (l/F)"+l  =  (l/F)"/2.0

                   or
                     if  (L/F)"*l   1.0,   (L/F)'"+l =  [l + (L/F)"I/2.0

                     This procedure eliminates most of the problems associated with flash calcula-
                   tions  in  single-phase regions  and  yields  excellent  results  in  relatively  few
                   iterations inside the two-phase region. Some problems still occur when attempt-
                   ing flash calculations in the dense gas regions.
                     Initial estimates of  the phase composition must be made to initiate the flash
                   calculation. Several procedures are available. It was  found that  a combination
                   of  the bubble point/dew  point initial phase estimation procedures works quite
                   well  [12]. Set the vapor phase mole fraction of  the highest component in the
                   system to  1.0 and the liquid phase mole fraction of  the heaviest component in
                   the  system  at  1.0. All  other  mole fractions are  set  to  loa.  This procedure is
                   believed to be superior to the technique of  basing the initial assumption of the
                   phase  composition on some  noncomposition dependent  K value  estimation
                   procedure, particularly when a wide range of temperatures, pressures, component
                   types, composition ranges, etc.,  is  to be considered.
                     The estimated vapor and liquid phase compositions must be compared with
                   the  calculated  phase  compositions.  Equations  6-19  and  6-23  describe  this
                   checking procedure.  If  the  restraints  described  by  these  equations  for  any
                   component (in either phase) are not satisfied, the calculations must be repeated
                   even  though an acceptable value for L/F  has been determined. Some feel that
                   this detailed checking procedure is unnecessary. It probably is unnecessary for
                   most problems involving moderate temperature-pressure-composition conditions.
                    However, at extreme conditions of temperature, pressure and composition (low-
                    temperatures, high-pressure, high-acid-gas compositions) failure to perform these
                    composition checks will  lead  to  results  that  are  completely incorrect  (poor
                    estimates of  the phase compositions and incorrect L/F  ratios). Unfortunately,
                    the boundary changes in temperature, pressure of  composition can completely
                    alter the difficulty of a given problem. Consequently, carehl application of these
                    checks in all calculations is strongly recommended since one can never be sure
                    that a particular problem will not fall into the area of  extreme conditions.
                     A logic diagram illustrating the basic flash calculation is shown in Figure 6-28.
                   All  the necessary features described earlier are embodied in this diagram.
                      Flash calculations at fixed L/F  and temperature or pressure are frequently
                    necessary.  In  these  calculations, the  dependent variable becomes pressure or
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