Page 223 - Bird R.B. Transport phenomena
P. 223

§7.5  Estimation of the Viscous Loss  207

                            Table  7.5-1  Brief  Summary  of Friction Loss Factors for  Use with  Eq. 7.5-10
                            (Approximate  Values for Turbulent Flow) fl

                            Disturbances                                  e v
                            Sudden changes in cross-sectional  area^
                            Rounded entrance to pipe                      0.05
                            Sudden contraction                         0.45(1  -  j8)
                            Sudden  expansion'                            - i

                            Orifice  (sharp-edged)                 2.71(1  -

                            Fittings and valves
                            90° elbows  (rounded)                        0.4-0.9
                            90° elbows  (square)                         1.3-1.9
                            45°  elbows                                  0.3-0.4
                            Globe valve (open)                           6-10
                            Gate valve (open)                             0.2

                            a
                             Taken from  H. Kramers, Physische Transportverschijnselen, Technische Hogeschool Delft, Holland (1958),
                            pp. 53-54.
                            b  Here (3 = (smaller cross-sectional area)/(larger  cross-sectional area).
                            c  See derivation  from the macroscopic balances in Example 7.6-1. If /3 = 0, then E  = \{v) , where (v) is the
                                                                                          2
                            velocity upstream from the enlargement.                  v


                               Most  flow  systems  contain various  "obstacles,"  such  as  fittings,  sudden  changes  in
                            diameter, valves, or flow measuring  devices.  These also  contribute to the friction  loss  E .
                                                                                                     v
                            Such additional resistances  may be written in the form  of  Eq. 7.5-4, with  e  determined by
                                                                                         v
                            one  of  two  methods: (a) simultaneous  solution  of  the macroscopic balances, or  (b) experi-
                            mental measurement. Some rough values  of e  are tabulated in Table  7.5-1  for  the conven-
                                                                  v
                            tion that (v) is  the average  velocity  downstream  from  the disturbance. These e  values  are
                                                                                             v
                            for  turbulent flow for  which the Reynolds number dependence is not too important.
                               Now  we  are in a position to rewrite  Eq. 7.4-7 in the approximate form  frequently  used
                            for  turbulent flow calculations in a system  composed  of various  kinds  of piping and addi-
                            tional  resistances:
                                                                             2
                                     M   - v\)                              v f  /) -   lv e    (7.5-10)
                                                                                         2
                                                                              ^h
                                                                       sum over all  /i  sum over all
                                                                       sections of  fittings, valves,
                                                                       straight conduits  meters, etc.
                            Here R h  is the mean hydraulic radius  defined  in Eq. 6.2-16,/is the friction  factor  defined
                            in  Eq. 6.1-4, and e  is the friction  loss factor  given  in Table  7.5-1. Note that the v x  and v 2  in
                                          v
                            the  first  term refer  to the velocities  at planes  1 and 2; the v in the first  sum  is the  average
                            velocity  in  the  zth pipe  segment;  and  the  v  in  the  second  sum  is  the  average  velocity
                            downstream from  the zth fitting, valve, or other obstacle.


        EXAMPLE  7.5-1      What  is the required power output from the pump at steady  state in the system  shown  in Fig.
                            7.5-1? The water  (p = 62.4 lb /ft ;  /л =  1.0  cp) is to be delivered  to the upper tank at a rate of
                                                     3
                                                   w
      Power  Requirement    12 ft /min.  All  of the piping is 4-in. internal diameter smooth circular pipe.
                               3
      for  Pipeline  Flow
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