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                                          Chapter 5
                                                   Water Hydraulics, Transmission, and Appurtenances






















                                     Figure 5.11 Moody diagram with the friction factor f, as a function of Reynolds number R, in Darcy–Weisbach formula for flow in
                                     conduits.

                                    where h is the head loss in ft (m) (energy loss because of  √
                                           f                                           R∕ f with scales for f and R added for convenience in
                                    surface resistance) in a pipe of length L in ft (m) and diame-  finding f for use in Eq. (5.10a).
                                    ter d in ft (m) through which a fluid is transported at a mean  In reference to R and   ∕r,:
                                                                           3
                                                                      3
                                    velocity v in ft/s (m/s) and flow rate Q in ft /s (m /s); g is the  1. Laminar flow persists until R = 2,000, and the f:R
                                                              2
                                                                       2
                                    acceleration of gravity, 32.2 ft/s (9.81 m/s ); f is a dimen-
                                                                                2  5         relationship is quite simply as follows:
                                    sionless friction factor (see Fig. 5.11); and K = 8fL∕   gd .
                                    In the more than 100 years of its existence, use, and study,              f = 64∕R           (5.12a)
                                    this formulation has been foremost in the minds of engineers
                                                                                             Reynolds number R and friction factor f are dimen-
                                    concerned with the transmission of water as well as other
                                                                                               sionless.
                                    fluids. That this has often been so in a conceptual rather than
                                                                                          2. Above R = 4,000, turbulent flow is fully established,
                                    a practical sense does not detract from its importance.
                                                                                             and the single trace for laminar flow branches into a
                                        Within Eq. (5.10a), the dimensionless friction factor f
                                                                                             family of curves for increasing values of   ∕r above
                                    is both its strength and its weakness in applications—its
                                                                                             a lower boundary that identifies the f:R relationship
                                    strength as a function of the Reynolds number R,
                                                                                             for smooth pipes as
                                                     R = vd  ∕   = vd∕         (5.11)
                                                                                                         √          √
                                                                                                       1∕ f = 2 log R f − 0.8     (5.13)
                                    where    is the absolute viscosity,    =   ∕   is the kinematic
                                    viscosity of the fluid, and    is its density; its weakness as  3. For rough pipes, the relative roughness   ∕r takes
                                    a function of relative roughness   ∕r, where    is a measure  command and
                                    of absolute roughness and r is the inside radius of the pipe          √
                                                                                                        1∕ f = 2 log r∕   + 1.74  (5.14)
                                    (2  ∕d =   ∕r). The f:R relationship is shown in Fig. 5.11, a
                                    general resistance diagram for flow in uniform conduits. This  where r is the radius of the pipe (ft or m) and   ∕r is
                                                                           √
                                    diagram evolves from a logarithmic plot of 1∕ f against    the relative roughness, dimensionless.
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