A weir in a horizontal channel is 1 m high and 4 m wide. The water depth upstream is 1.6 m. Estimate the discharge if the weir is (a) sharp-crested and (b) round-nosed with an unfinished concrete broad crest 1.2 m long. Neglect V_1^2/(2g).
A weir in a horizontal channel is 1 m high and 4 m wide. The water depth upstream is 1.6 m. Estimate the discharge if the weir is (a) sharp-crested and (b) round-nosed with an unfinished concrete broad crest 1.2 m long. Neglect V_1^2/(2g).
Part (a)
We are given Y = 1 m and H + Y ≈ 1.6 m, hence H ≈ 0.6 m. Since H \ll b, we assume that the weir is “wide.” For a sharp crest, Eq. (10.56) applies:
Wide sharp-crested weir: C_d \approx 0.564 + 0.0846 \frac{H}{Y} for \frac{H}{Y} \leq 2 (10.56)
C_d \approx 0.564 + 0.0846 \frac{0.6 m}{1 m} \approx 0.615Then the discharge is given by the basic correlation, Eq. (10.55):
Q_{weir} = C_db \sqrt{g} \left(H + \frac{V^2_1}{2g}\right)^{3/2} \approx C_db \sqrt{g}H^{3/2} (10.55)
Q = C_db \sqrt{g}H^{3/2} = (0.615)(4 m) \sqrt{(9.81 m/s^2)}(0.6 m)^{3/2} \approx 3.58 m^3/sWe check that H/Y = 0.6 < 2.0 for Eq. (10.56) to be valid. From continuity, V_1 = Q/(by_1) = 3.58/[(4.0)(1.6)] = 0.56 m/s, giving a Reynolds number V_1H/ \nu \approx 3.4 E5.
Part (b)
For a round-nosed broad-crested weir, Eq. (10.57) applies. For an unfinished concrete surface, read ε ≈ 2.4 mm from Table 10.1. Then the displacement thickness is
Round-nosed broad-crested weir: C_d \approx 0.544 \left(1 – \frac{\delta^*/L}{H/L}\right)^{3/2} (10.57)
\frac{\delta^*}{L} \approx 0.001 + 0.2 \sqrt{\epsilon /L} = 0.001 + 0.2 \left(\frac{0.0024 m}{1.2 m}\right)^{1/2} \approx 0.00994Table 10.1 Experimental Values of Manning’s n Factor^* | Average roughness height ε |
||
n | ft | mm | |
Artificial lined channels: | |||
Glass | 0.010 ± 0.002 | 0.0011 | 0.3 |
Brass | 0.011 ± 0.002 | 0.0019 | 0.6 |
Steel, smooth | 0.012 ± 0.002 | 0.0032 | 1 |
Painted | 0.014 ± 0.003 | 0.008 | 2.4 |
Riveted | 0.015 ± 0.002 | 0.012 | 3.7 |
Cast iron | 0.013 ± 0.003 | 0.0051 | 1.6 |
Concrete, finished | 0.012 ± 0.002 | 0.0032 | 1 |
Unfinished | 0.014 ± 0.002 | 0.008 | 2.4 |
Planed wood | 0.012 ± 0.002 | 0.0032 | 1 |
Clay tile | 0.014 ± 0.003 | 0.008 | 2.4 |
Brickwork | 0.015 ± 0.002 | 0.012 | 3.7 |
Asphalt | 0.016 ± 0.003 | 0.018 | 5.4 |
Corrugated metal | 0.022 ± 0.005 | 0.12 | 37 |
Rubble masonry | 0.025 ± 0.005 | 0.26 | 80 |
Excavated earth channels: | |||
Clean | 0.022 ± 0.004 | 0.12 | 37 |
Gravelly | 0.025 ± 0.005 | 0.26 | 80 |
Weedy | 0.030 ± 0.005 | 0.8 | 240 |
Stony, cobbles | 0.035 ± 0.010 | 1.5 | 500 |
Natural channels: | |||
Clean and straight | 0.030 ± 0.005 | 0.8 | 240 |
Sluggish, deep pools | 0.040 ± 0.010 | 3 | 900 |
Major rivers | 0.035 ± 0.010 | 1.5 | 500 |
Floodplains: | |||
Pasture, farmland | 0.035 ± 0.010 | 1.5 | 500 |
Light brush | 0.05 ± 0.02 | 6 | 2000 |
Heavy brush | 0.075 ± 0.025 | 15 | 5000 |
Trees | 0.15 ± 0.05 | ? | ? |
^*A more complete list is given in Ref. 2, pp. 110–113.
Then Eq. (10.57) predicts the discharge coefficient:
C_d \approx 0.544 \left(1 – \frac{0.00994}{0.6 m/1.2 m}\right)^{3/2} \approx 0.528The estimated flow rate is thus
Q = C_db \sqrt{g}H^{3/2} = 0.528(4 m) \sqrt{(9.81 m^2/s)}(0.6 m)^{3/2} \approx 3.07 m^3/sCheck that H/L = 0.5 < 0.7 as required. The approach Reynolds number is V_1H/ \nu \approx 2.9 E5, just barely below the recommended limit in Eq. (10.57).
Since V_1 ≈ 0.5 m/s, V^2_1/(2g) ≈ 0.012 m, so the error in taking total head equal to 0.6 m is about 2 percent. We could correct this for upstream velocity head if desired.