Fluid mechanics, open water channel velocity - bernoulli & conservation of flow

AI Thread Summary
In an open water channel with a small bump, the relationship between the fluid heights and velocities can be expressed through Bernoulli's equation and the conservation of flow. The equation h1 = Δh + H + h2 describes the water level above the bump, where Δh is the dip caused by the bump's height H. The velocity v2 directly above the bump can be derived as v2 = [2gΔh / ((h1/h2)^2 - 1)]^(1/2), assuming no energy losses. The discussion emphasizes the need to manipulate the conservation of mass and energy principles to find the velocity expression. This analysis is crucial for understanding fluid dynamics in open channel flow.
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Homework Statement



If in an open water channel, the approach speed of an incompressible ideal fluid, of constant depth h1, is not too large, a small bump in height H (H<< h1) in the base of the channel will cause a dip Δh (Δh << H) in the water level directly above it, such that h1 = Δh + H + h2, where h2 is the height of the fluid above the bump.

Under these conditions, such an arrangement can be used for measuring the flow velocity

Q. Assuming no losses, show that the velocity v2, directly above the bump is given by

v_2 = [\frac{2gΔh} {(\frac{h1}{h2})^2 - 1}]^\frac{1}{2}



Homework Equations



0.5*u^2 + gh_1 = 0.5* v_2^2 + g(h_2 + H)<br /> <br /> g (h_1 - (H + h_2) = 1/2 (v_2^2 - u^2) = g \delta h


The Attempt at a Solution



We want the expression for v_2

v_1h_1 = v_2h_2------->v_1 = \frac {v_2h_2}{h_1}

Thanks for the help!
 
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