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Laminar flow, mechanical energy balanc

This is the mechanical-energy loss due to skin friction for the pipe in N m/kg of fluid and is part of the F term for frictional losses in the mechanical-energy-balance equation (2.7-28). This term (Pi—Pz)/ for skin friction loss is different from the (p, — Pz) term, owing to velocity head or potential head changes in Eq. (2.7-28). That part of F which arises from friction within the channel itself by laminar or turbulent flow is discussed in Sections 2.10B and in 2. IOC. The part of friction loss due to fittings (valves, elbows, etc.), bends, and the like, which sometimes constitute a large part of the friction, is discussed in Section 2.10F. Note that if Eq. (2.7-28) is applied to steady flow in a straight, horizontal tube, we obtain (pi — Pz)/p = F. [Pg.85]

Kinetic energy in laminar flow. In application of the total mechanical-energy balance in Eq. (2.7-28), the average kinetic energy per unit mass of fluid is needed. For fluids, this is (S2)... [Pg.159]


See other pages where Laminar flow, mechanical energy balanc is mentioned: [Pg.638]    [Pg.643]    [Pg.12]    [Pg.17]    [Pg.463]    [Pg.468]    [Pg.438]    [Pg.429]    [Pg.785]    [Pg.790]    [Pg.186]    [Pg.793]    [Pg.798]    [Pg.642]    [Pg.647]    [Pg.74]    [Pg.140]    [Pg.157]    [Pg.74]    [Pg.234]    [Pg.1127]   
See also in sourсe #XX -- [ Pg.186 ]




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