Losses and Friction Factors
- Over a finite length l , the head loss
(26.11)
Combining Eqs (26.10) and (26.11), we get
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or  |
(26.12) |
- On the other hand, the head loss in a pipe flow is given by Darcy-Weisbach formula as
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(26.13) |
where "f" is Darcy friction factor . Equations (26.12) and (26.13) yield
which finally gives , where is the Reynolds number.
- So, for a fully developed laminar flow, the Darcy (or Moody) friction factor is given by
Alternatively, the skin friction coefficient for Hagen-Poiseuille flow can be expressed by
With the help of Eqs (26.9b) and (26.9c), it can be written
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(26.14b) |
The skin friction coefficient Cf is called as Fanning's friction factor . From comparison of Eqs (26.14a) and (26.14b), it appears
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- For fully developed turbulent flow, the analysis is much more complicated, and we generally depend on experimental results. Friction factor for a wide range of Reynolds number (104 to 108) can be obtained from a look-up chart . Friction factor, for high Reynolds number flows, is also a function of tube surface condition. However, in circular tube, flow is laminar for Re ≤ 2300 and turbulent regime starts with Re ≥ 4000.
- The surface condition of the tube is another responsible parameter in determination of friction factor.
- Friction factor in the turbulent regime is determined for different degree of surface-roughness
of the pipe, where is the dimensional roughness and Dh is usually the hydraulic diameter of the pipe .
- Friction factors for different Reynolds number and surface-roughness have been determined experimentally by various investigators and the comprehensive results are expressed through a graphical presentation which is known as Moody Chart after L.F. Moody who compiled it.
- The hydraulic diameter which is used as the characteristic length in determination of friction factor, instead of ordinary geometrical diameter, is defined as
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(26.15) |
where Aw is the flow area and Pw is the wetted perimeter .
- Kinetic energy correction factor ,
The kinetic energy associated with the fluid flowing with its profile through elemental area and the total kinetic energy passing through per unit
time .
- This can be related to the kinetic energy due to average velocity(
), through a correction factor, α as 
or  |
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- Here, for Hagen-Poiseuille flow,
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(26.16) |
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