Page 215 - APPLIED PROCESS DESIGN FOR CHEMICAL AND PETROCHEMICAL PLANTS, Volume 1, 3rd Edition
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Pumping of Liquids                                       187

               units and the discharge head must be calculated in   Discharge Head, hd
               absolute units.
            5. Suction lift is a negative suction head, S, used to des-   The discharge head of a pump is the head measured at
               ignate a negative static condition  on the suction of   the  discharge  nozzle  (gauge or  absolute), and  is  com-
               the pump (below atmospheric). The sign for suction   posed of the same basic factors previously summarized; 1.
               head is positive (+) , while its corresponding termi-   static head 2.  friction  losses through  pipe, fittings, con-
               nology of suction lift is negative (-),  since the term   tractions, expansions, entrances and exits 3. terminal sys-
               “lift” denotes a negative condition. Note that the only   tem pressure.
               difference in these terms is the difference in signs.   Some typical discharge systems are given in Figure 3-
                                                                42. General practice is to express the terminal discharge
            This applies because the total head for a pump is total   pressure, P, at a vessel as in Figure 3-42 in terms of gauge
          discharge  head  a(+), minus  (-)  the  [suction  head,   pressure, and hence P = 0 for atmospheric discharge. If P
          a(+)], or [suction lifit, a(-)].                      is  less  than  atmospheric  or  otherwise  expressed  in
            For  general  service  the  average  centrifugal  pump   absolute units, then it must be added a3 equivalent feet of
          should lift about 15 feet of water on its suction side. How-   liquid to the value of hd ordinarily expressed as a gauge
          ever, since each process situation is different, it is not suf-   reading.
          ficient to assume that a particular pump will perform the   Figures 3-38 and 3-39 illustrate the use of siphon action
          needed suction lift. ALctually, certain styles or models of a   in  pump  systems. Theoretically, the  head  in  the  siphon
          manufacturer‘s pumps are often specially adapted to high   should be recoverable, but actually it may no~, at least not
          lift  conditions.  On the  other  hand  it  is  unnecessary  to   equivalent foot for foot. Usually not more than 20 feet of
          select a high  lift pump when  pressure  head  or flooded   siphon action can be included [4] even though 34 feet are
          suction  conditions prevail. Proper  evaluation of  suction   theoretical at sea level. The siphon length is D’ in the fig-
          lift conditions cannot be over emphasized.            ures  [32]. For  some systems the  discharge head  on the
            The theoretical maximum  suction lift at sea level for   pump should be used as (I3 + D’) , neglecting the siphon
          water (14.7 psi) (2.31 ft/psi)  = 34 ft. However, due to flow   action. In any case, if air can be trapped in the loop, (and
          resistance, this value 11s  never attainable. For safety, 15 feet   it usually can) it must be vented during start-up, otherwise
          is con sidered the  pr,actical limit,  although  some pumps   the pump will be pumping against the head established
          will lift somewhat higher cotumns of water. When sealing   using  (D  + D’).  On  start-up the  flow can  be  gradually
          a vacuum condition  above a pump, or the pump pumps   increased, making more head available from the pump to
          from  a vessel, a seal allowance  to  atmosphere  is  almost   overcome  the  higher  starting  head  of the  system. This
          always taken as 34 feet of water. High suction lift causes a   should not be  overlooked nor underestimated  in  deter-
          reduction  in  pum  capacity,  noisy  operation  due  to   mining the specifications for the pump.
          release of air and vapor bubbles, vhation and erosion, or
          pitting (cavitation) of the impeller and some parts of the   Velocity Head
          casing. (The extent of the damage depends on the mate-
          rials of construction.)                                 Velocity head is the kinetic energy of a liquid as a result
                                                                of its motion at some velocity, v.  It is the equivalent head




                                                               Atmospheric
                                                                Pressure
                         Entrance Loss (EL)



                                                     Pump                    Pump
                                                                                hd  =  D + hdL
                                                                                        (c9
                          Note: For  a  system  evaluation, including  suction  and  discharge, the  units  of  P must  be  the  same
                              either  gage  or  absolute ,expressed  as  feet  of  fluid.
                              The  friction losses from  the  pump  to  the  vessel include any entrance  or exit  Iosses.Un!ess
                              velocities  are  high, these  losses  are usually negligible.
                                               Figure 3-42. Typical discharge systems.
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