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4.  For vertical separators, liquid droplets (oil) separate by settling
                     downward against an up-flowing gas stream; for horizontal
                     ones, liquid droplets assume a trajectory like path while it flows
                     through the vessel (the trajectory of a bullet fired from a gun).
                 5.  For vertical separators, the gas capacity is proportional
                     to the cross-sectional area of the separator, whereas for
                     horizontal separators, gas capacity is proportional to area of
                     disengagement (LD) (i.e., length   diameter).


            3.6.3  Settling of Oil Droplets
            In separating oil droplets from the gas in the gravity settling section of a
            separator, a relative motion exists between the particle, which is the oil
            droplet, and the surrounding fluid, which is the gas.
                 An oil droplet, being much greater in density than the gas, tends to
            move vertically downward under the gravitational or buoyant force, F g .
            The fluid (gas), on the other hand, exerts a drag force, F d , on the oil
            droplet in the opposite direction. The oil droplet will accelerate until the
            frictional resistance of the fluid drag force, F d , approaches and balances
            F g ; and, thereafter, the oil droplet continues to fall at a constant velocity
            known as the settling or terminal velocity.
                 The drag force, F d , is proportional to the droplet surface area
            perpendicular to the direction of gas flow, and its kinetic energy per unit
            volume. Hence,
                           2    g u 2
                 F d ¼ C d  d                                             ð1Þ
                        4    2
            whereas F g is given by
                        3
                 F g ¼  d ð  o     g Þg                                   ð2Þ
                     6
            where C d is the drag coefficient, d is the diameter of the oil droplet (ft), u is
            the settling velocity of the oil droplet (ft/s),   o and   g are the oil and gas
                                                                         2
                         3
            densities, (lb/ft ), respectively, and, g is gravitational acceleration (ft/s ).
                 The settling terminal velocity, u, is reached when F d ¼ F g . Therefore,
            equating Eqs. (1) and (2) and solving for u, the droplet settling velocity, we
            obtain

                  2  8 ð  o     g Þ  d
                 u ¼ g
                     6      g    C d
            The droplet diameter d is normally expressed in microns, where 1 mmis
            equal to 3.2808   10  6  ft. Let d m be the droplet diameter (in mm) and






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