Page 90 - Handbook Of Multiphase Flow Assurance
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Flow modeling                              85

            TABLE 4.4  Application of correlations to flow in cylindrical pipes
            Correlation                              Geometry   Development  Observation
            Beggs-Brill (Beggs and Brill, 1973)      Inclined   Empirical
            Duns-Ross (Duns Jr. and Ros, 1963)       Vertical   Empirical
            Hagedorn-Brown (Hagedorn and Brown, 1965)  Vertical  Empirical   Small diameter
            Mukherjee-Brill (Mukherjee and Brill, 1985)  Inclined  Empirical
            Dukler (Dukler et al., 1964)             Vertical   Mechanistic  Holdup model issues
            Aziz (Aziz et al., 1972)                 Vertical   Mechanistic


            the flow modeling today is performed using software. Discussion and review of various flow
            correlations is available in literature such as (Brill and Mukherjee, 1999).
              To name a few correlations as in Table 4.4 and their typical application to flow in cylindri-
            cal pipes,
              A more detailed information on flow correlation is in the chapter on reference information.
              Although each correlation had been fit to best accuracy to data available at the time,
            broader application of two-phase flow correlations may provide ±50% accuracy in system
            with different conditions.
              At present both engineering firms and academia aim to use computational power to val-
            idate three-phase correlations against ever larger data sets, including tens of thousands of
            flow cases (Roullier et al., 2017). This results in a more reliable predictive capability of soft-
            ware tools and more cost-effective production system design.


            Dimensionless numbers
              The dimensionless numbers more commonly used in flow assurance as in multiphase flow,
            fluid interfaces or solids deposition modeling include:


                                                  ρvD   inertialforce
                                    Reynolds Re =      =
                                                   µ    viscousforce

                                               µ     momentum  diffusion
                                 Prandtl Pr =      =
                                               /
                                             kC  P    thermal  diffusion

                                                v       inertialforce
                                 Froude Fr =        =
                                             ( gD) 05 .  gravitationalforce

                                     v         compressible fluid velocity
                        Mach Ma =        =
                                    v      speed of     inncompressible fluid
                                                 sound
                                     Sound
                              ∆ P   pressure  o frce
                   Euler Eu =     =             =  energydissipatioon in fluid flow

                              ρ v 2  inertialforce
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