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Question 12.7: The flow in the 2-m-wide channel in Fig. 12–16a is controlle......

The flow in the 2-m-wide channel in Fig. 12–16a is controlled by the sluice gate, which is partially opened so that it causes the depth of the water near the gate to be 3 m and the mean velocity there to be 0.5 m/s. Determine the depth of the water far upstream, where it is essentially at rest, and also find its depth downstream from the gate where free outflow occurs.

fig 12-16a
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Fluid Description.   The water a distance far upstream from the sluice gate is assumed to have a constant depth so that the flow at points 1 and 2 will be steady. Also, the water is assumed to be an ideal fluid.

Analysis.   If the Bernoulli equation is applied between points 0 and 1, located on a streamline at the water surface, we have

\frac{p_0}{\gamma}  +  \frac{V_0^2}{2g}  +  y_0  =  \frac{p_1}{\gamma}  +  \frac{V_1^2}{2g}  +  y_1

 

0  +  0  +  y_0  =  0  +  \frac{(0.5  m/s)^2}{2(9.81  m/s^2)}  +  3  m

 

y_0 = 3.01274 m = 3.0127 m

The Bernoulli equation can be applied between points 1 and 2, but we can also apply it between points 0 and 2. If we do this, we have

\frac{p_0}{\gamma}  +  \frac{V_0^2}{2g}  +  y_0  =  \frac{p_2}{\gamma}  +  \frac{V_2^2}{2g}  +  y_2

 

0  +  0  3.01274  m  =  0  +  \frac{V_2^2}{2(9.81  m/s^2)}  +  y_2                     (1)

Continuity requires the flow at 1 and 2 to be the same.
Q  =  V_1A_1  =  V_2A_2

(0.5  m/s)[3  m (2  m)]  =  V_2 y_2(2  m)

 

V_2y_2  =  1.5

Substituting V_2 = 1.5/y_2 into Eq. 1 yields
y_2^3  –  3.01274y_2^2  +  0.11468  =  0
Solving for the three roots, we get
y_1  =  3  m                  Subcritical (as before)
y_2  =  0.2020  m       Supercritical
y_2  =  -0.1892  m       Not realistic
The first root indicates the depth y_2  =  y_1 = 3 m, and the second root is the depth downstream from the gate. Thus,

y_2 = 0.202 m
The specific energy for the flow can be determined either from point 0, 1, or 2 since the bed elevation of the channel is constant and friction losses through the gate have been neglected (ideal fluid). Using point 1,

E  =  \frac{q^2}{2gy_2^2}  +  y_2  =  \frac{[(0.5  m/s) (3  m)]^2}{2(9.81  m/s^2)(3  m)^2}  +  3  m  =  3.01274  m

A plot of the specific energy is shown in Fig. 12–16b. Here

y_c  =  \frac{2}{3} y_0  =  \frac{2}{3}(3.01274  m)  =  2.0085  m

 

E_{min}  =  \frac{q^2}{2gy_c^2}  +  y_c  = \frac{[(0.5  m/s)(3  m)]^2}{2(9.81  m/s^2)(2.0085  m)^2}  +  2.0085  m  =  2.037  m

As noted, subcritical flow occurs upstream near the gate, and supercritical flow occurs downstream.

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