Page 66 - Applied Process Design for Chemical and Petrochemical Plants Volume I
P. 66

54                        Applied Process Design for Chemical and Petrochemical Plants
















                                                     gauge    valve
                          Spira-tec trap _I   t
                          leak indicator

                                 Figure 2-2. Portion of a plant piping system. By permission, Spirax-Sarco, Inc., 1991.


               The many empirical  correlations  advanced  to  repre-   conditions. If  these criteria do not apply, then refer
             sent  the  frictional  resistance  to  flow  vary  from  exact   to the method using the flow coefficient, K
             results  because  of  the  specific  simplifylng assumptions   3. For larger pressure drops in long lines of a mile or
             incorporated in each. Some relations agree in one region   greater  in  length  than  noted  above, use  methods
             of flow and diverge in others.                            presented with  the Weymouth, Panhandle Gas for-
                                                                       mulas, or the simplified compressible flow equation.
                    Compressible Flow: Vapors and Gases (31
                                                                     4. For isothermal conditions [3]:
               Compressible  fluid  flow  occurs  between  the  two
             extremes of isothermal and adiabatic conditions. For adia-
             batic  flow  the  temperature  decreases  (normally)  for
             decreases in pressure, and the condition is represented by   w,  =                      -
             p’V’ck) = constant. Adiabatic flow is often assumed in short        L
             and well-insulated pipe,  supporting the  assumption that           D
             no heat is transferred to or from the pipe contents, except   lbs/sec                               (2 - 3)
             for  the  small  heat  generated  by  friction  during  flow.
             Isothermal p’Va = constant temperature, and is the mech-
             anism usually (not always) assumed for most process pip-         /I                  1
             ing design. This is in reality close to actual conditions for
             many process and utility service applications.
               The single-phase friction loss (pressure drop) for these
             situations  in  chemical  and  petrochemical  plants  is  still
             represented  by  the  Darcy equation  with  specific limita-   lbs/sec                              (2 - 4)
             tions [3]:

               1. If calculated pressure drop from inlet (upstream) to   The correlations included here are believed to apply to
                 outlet  (downstream)  of  a  line  system  is  less  than   good  plant  design  procedures  with  good  engineering
                 about 10% of inlet pressure PI, reasonable accuracy
                                                                   accuracy.  As  a matter of good practice with the exercise of
                 can be expected provided the specific volume used   proper judgment, the designer should familiarize himself
                 is based on inlet or outlet conditions.           with the background of the methods presented in order
               2. If calculated pressure drop from inlet to outlet of line   to better select the conditions associated with  a specific
                 system  (not including  control  or  hand  valves)  is   problem.
                 greater than approximately lo%, but less than about
                 40% of the inlet pressure PI (pounds per square inch   Design conditions may be:
                 gauge),  the  Darcy  equation  will  yield  reasonable
                 accuracy when using a specific volume based on the   1. Flow  rate  and pressure  drop allowable established,
                 average of upstream (inlet) and downstream (outlet)   determine pipe size for a fixed length
   61   62   63   64   65   66   67   68   69   70   71