Page 108 - Petroleum and Gas Field Processing
P. 108

Rearrange Eq. (20) to solve for Q o :
                                    2  !
                                  D L    2
                         Q ¼ 0:7       D L
                           o
                                    t
                    Substitute L o ¼ 10.5 and D ¼ 36 in the above equation and solve
                    for Q o :
                         Q ¼ 3:176 bbl=day
                           o
            Comparing the above actual oil and gas capacities to the design production
            rates of Example 3 shows that the separator can handle almost five times the
            design gas rate of Example 3. This is because the cross-sectional area for gas
            flow is much more than needed for settling. In such situations, it is evident
            that the assumption of allowing each phase to occupy one-half of the
            separator effective volume is not a good assumption. The size of the
            separator could certainly be reduced if the design was based on allowing
            the gas to flow through a smaller area than the 50% of the total area. It is
            recommended that the reader solve this problem assuming the gas to occupy
            a smaller volume than 50% of the separator volume. Care must be taken in
            modifying the above design equations used.
                 Geometrical relationships relating the cross-sectional area occupied
            by the gas, the height of the gas column, and the vessel diameter could
            be derived. For the cases where the cross-sectional area of the gas flow,
            A g , is not equal to one-half of the vessel cross-sectional area, A; that is, the
            height of the gas, H g , is not equal to the radius, D/2, Lockhart [6]
            presented the following simplified, but reasonably accurate, relationships.

                 (a)  To determine H g /D as a function of A g /A:
                     0   A g /A   0.2:
                                                 2            3

                         H g       A g        A g         A g
                            ¼ 2:481     12:29     þ31:133
                          D         A         A            A
                     0.2   A g /A   0.8:
                         H g        A g
                            ¼ 0:8123   þ 0:0924
                          D          A
                     0.8   A g /A   1.0:
                                                                 2

                              H g             A g            A g
                           1       ¼ 2:481 1        12:29 1
                               D              A               A
                                                    3

                                                 A g
                                    þ 31:133 1
                                                 A



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