Page 175 - Pipeline Rules of Thumb Handbook
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162     Pipeline Rules of Thumb Handbook

         Weight basis:                                           To correct for deviation from the universal gas law, the
                                                               compressibility factor is inserted in Equation 11, becoming:
                                È 3417  D P ˘
               .
          W = 106  dP ZC C C v1  1  2  sin Í  ˙ Deg.    (10)    C v = (    )        P P )
                                Î  CC 2  P ˚                         Q 1360  G TZ (D  ¥  2                    (12)
                                                                               b
                                        1
                                  1
           The C 1 factor in Equations 9 and 10 is currently available  On a weight basis, this equation becomes:
         from Fisher Controls for their valves. Other companies pre-
                                                                                   ¥
         sumably do not publish this factor. (The C 2 factor is shown in  C v = ( W 104 )  TZ (D P P ¥ G b )  (13)
                                                                                     2
         Figure 4.)
                                                                 Mixed phase flow. Mixed phase flow is generally experi-
                                                               enced when:

                                                                 1. Liquid entrainment is carried by a gaseous flow.
                                                                 2. Liquid at or near its boiling point vaporizes as it flows
                                                                    through a line and its restrictions.

                                                                 In the discussion under “Flashing Service,” it is explained
                                                               that flashing can be reduced or eliminated by limiting the DP
                                                               across the valve. When two-phase flow already exists or when
                                                               it occurs in the control valve, two methods are given to size
                                                               the valve.

                                                                 1. A rule of thumb that has been used for years is to cal-
                                                                    culate the C v based on liquid only and increase the valve
                                                                    body to the next size. This is satisfactory in many cases,
                                                                    but it obviously does not take into account varying ratios
                                                                    of liquid to vapor.
                                                                 2. A preferred method is to determine the amount of vapor
                                                                    and liquid, then calculate and add the C v of each phase
                                                                    to get the overall C v requirement. The percent vapor-
         Figure 4. The C 2 factor is applicable only to Equations 9 and  ization can be calculated by the responsible engineer if
         10, the Fisher universal equations for gas and vapor flows.
                                                                    it is not furnished by the process people.



                                                                 Example.
           An equation for gases and vapors proposed by the Foxboro
         Company (Foxboro TI Bulletin 31-4K) is identical with the  Fluid—Propane
         FCI equation, except that P 2 is used instead of (P 1 + P 2)/2:  100gpm @ 300°psia and 130°F
                                                               s.g. @ 130°F = 0.444
          C v = ( Q 1360 )  GT D P P ()                 (11)   s.g. @ 60°F = 0.5077
                              2
                                                               s.g. @ P 2 (200psia) = 0.466 @ 104°F
           A comparison of the Fisher Universal, FCI, and Foxboro  DP = 100psi
         equations is made in the TI Bulletin 31-4K. A plot is given  % vaporization = 15.05%
         showing the results of these three equations using the same  M.W. = 44
         data (Figure 5).                                      Z = 0.8
           The Foxboro equation gives C v values essentially the same  G b = 44/29 = 1.518
                                                               Flow = 100gpm ¥ 0.444 = 22,200lb/hr
         as the universal equation at pressure drops up to 25% of P 1
         and gives 7% larger values at a pressure drop of 50% of P 1.  Vapor = 22,200 ¥ 0.1505 = 3,340lb/hr
         At the higher end of DP/P 1 ratios, a slightly larger valve should  Liquid = 22,200 - 3,340 = 18,860lb/hr
         be helpful to allow for the expanding vapors. The same agree-
         ment is claimed for steam flows although no plot is given.  Using Equation 13:
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