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                    162  Chapter 5  Water Hydraulics, Transmission, and Appurtenances


                                         Solution 2 (SI System):
                                             Velocity, v   Q>A
                                                               3
                                                                          2
                                                       (0.0445 m /s)>[(0.300 m)   0.785]
                                                       0.62 m/s
                                             Reynolds number, R   vd >
                                                                                             3
                                                                                                       2
                                                               (0.62 m/s)(0.300 m)(0.851   1,000 kg/m )>(0.1 N-s/m )
                                                               1,580   2,000, which indicates a laminar flow
                                             Friction factor, f   64>R
                                                            64>1,580
                                                            0.041
                                                                2
                                             Head loss, h f   f(L>d) (v >2g)
                                                                                               2
                                                                                   2
                                                         (0.041)(3,048 m/0.300 m)(0.62 m/s) >(2   9.81 m/s )
                                                         8.2 m






                     EXAMPLE 5.3   RATIO OF HEAD LOSS IN A PIPE TO THAT IN A PERFORATED PIPE
                                         Show that the head loss h f in a pipe is equal to three times the head loss h f in a perforated pipe,
                                         having the same length, diameter, and friction factor.
                                             Take the flow in the unperforated pipe as Q 0 ; assume a straight-line variation of the flow Q
                                         with distance in the perforated pipe, with Q   Q 0 at the inlet of the pipe and Q   0 at the end of
                                         the line. Consider only losses to pipe friction, and assume no variation in the value of f with a
                                         changing Q.

                                         Solution:
                                                                       2
                                                              h f   f(L>d)(v >2g)                          (5.10a)
                                          Since               v   Q>A                                        (5.4)
                                                                             2
                                                                         2
                                          Then                h f    f (L>D) (Q >2gA )                      (5.16)
                                                                           2
                                                                             2
                                                              h f    ( f>D)(1>2gA )Q L                      (5.17)
                                                                    2
                                                              h f    KQ L
                                                                           2
                                          Where               K   ( f>D)(1>2gA )
                                                                        dx

                                                           Q 0
                                                                                              Q x



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