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<br />EM 1110-2-1416 <br />15 Oct 93 <br /> <br />'"' <br /> <br />v <br /> <br />, <br /> <br /> <br />~ <br /> <br />, ' <br /> <br />tAMlNAR OPEN C~NEL <br />fLOW VELOCITY PROFlLE <br /> <br />/ " <br /> <br />'/ <br /> <br />, <br /> <br /> <br />,~ ,,' <br /> <br />-..:" ,,,< <br /> <br />LAIoI1NAR PIPE fLOW <br />VELOCITY PROFILE <br /> <br />Figure 2-2. laminar and turbulent velocity profilas <br /> <br />should refer to texts by Chow (1959), Henderson (1966), <br />and Rouse (1959). <br /> <br />c. Effects of gravity (subcritical and supercritical <br />flow). The ratio of inertial to gravitational forces is an <br />important measure of the state of open channel flow and <br />is represented by the Fronde number: <br /> <br />F~~ <br />IiL <br /> <br />(2-2) <br /> <br />where <br /> <br />F = Froude number (dimensionless) <br />V = mean flow velocity in the channel (ft/sec) <br />g = acceleration of gravity (ftlsec2) <br />L = characteristic length term (ft) <br /> <br />In open charmels and rivers the characteristic length (L) <br />is often taken as the hydraulic depth; i.e., the <br />cross-sectional area normal to the flow divided by the top <br />width at the free surface. Depending on the magnitude <br />of the Fronde number, the state of flow is either "sub- <br />critical', "criticar', or "supercriticaI." <br /> <br />2.6 <br /> <br />v <br /> <br />, ,,< <br /> <br />, <br /> <br />TURBULENT OPEN CHANNEL <br />fLOW VELOCITY PROFILE <br /> <br />, '/ <br /> <br /> <br /> <br />, . <br /> <br />-..:" ,Y <br /> <br />TURBULENT PIPE FLOW <br />VELOCITY PROFlLE <br /> <br />(I) When the Fronde number is less than 1, the <br />effects of gravitational forces are greater than inertial <br />forces, and the state of the flow is referred 10 as subcriti- <br />cal, or tranquil flow. Note that the denominalor in the <br />Froude number (Equation 2-2) is the expression for celer- <br />ity of a shallow water wave. Therefore, in subcritical <br />flow, the wave celerity is greater than mean channel <br />velocity, and a shallow water wave can move upstream. <br />As a simple field test, toss a slone into the river; if you <br />observe the ripples from the stone hitting the water mov- <br />ing upstream, the flow for that location, depth, and dis- <br />charge is subcritical (F < I). <br /> <br />(2) When inertial and gravitational forces are equal, <br />the Froude number is equal 10 unity, and the flow is said <br />to be at the critical state (i.e., critical flow). For these <br />conditions, a shallow water wave remains approximately <br />stationary in the flow relative to the banks. At critical <br />flow, the depth is referred 10 as "critical depth." <br /> <br />(3) When inertial forces exceed gravitational forces <br />(F > I) the state of flow is referred to as supercritical, or <br />rapid flow. For this state, the flow is characterized by <br />high velocity, and shallow water waves are immediately <br /> <br />e <br /> <br />. <br />, <br /> <br />.. <br />. <br /> <br />e <br /> <br />1 <br /> <br />. <br /> <br />e <br />