The upstream design pool elevation [HW elevation] is = 112 - 2 = 110 ft.
The downstream invert elevation is z2 = 100 - (So L) = 100 - (0.02 × 200) = 96 ft.
The downstream pool elevation [TW elevation] is = 96 + 4 = 100 ft.
First assume outlet control, and apply the energy equation between u/s and d/s. Velocities are zero in the u/s and d/s pools.
110 = 100 + [Ke + KE + f (L/D)] [V2/(2g)]
10 = [0.5 + 1.0 + 0.015 (200/D)] [V2/(2g)]
[V2/(2g)] = Q2/ { [(π/4)D2]2 2g } = (220)2/(0.6168 × 64.4 × D 4)
= 1218 / D4
10 = [1.5 + (3/D)] (1218 / D4)
Solve by trial and error: D = 4.1 ft. Assume D = 4.5 ft = 54 in.
From Fig. 7-5, HW/D = 2.4
HW depth = 2.4 × 4.5 = 10.8 ft.
HW elevation = 100 + 10.8 = 110.8 ft. [Too high!]
Next assume D = 5 ft.
From Fig. 7-5, HW/D = 1.7
HW depth = 1.7 × 5 = 8.5 ft.
HW elevation = 100 + 8.5 = 108.5 ft. [OK]
Check critical depth: Q / (g1/2do5/2) = 220 / [(32.2)1/2 (5)5/2] = 0.69
From Fig. 4-15: yc / do = 0.85
yc = 4.25 ft.
Calculate normal depth: (Q n) / (1.49 S1/2 do8/3) =
(220 × 0.013) / (1.49 × 0.14142 × 73.1) = 0.19
yn / do = 0.55
yn = 2.75 ft.
The flow is supercritical.
Since TW = 4 < yc = 4.25, there will be no hydraulic jump in the culvert.
Since the outlet is open to the atmosphere, there is inlet control.
Do/D1 = 24 / 8 = 3
The pressure coefficient is defined as: V1 = Vo (1 - Cp)1/2
Cp = 1 - (V1/Vo)2 = 1 - (Do/D1)4 = - 80
The free-vortex incipient cavitation index is: σi, A = 1 - 2 Cp = 1 - [2 × (- 80)] = 161
pv = 37 psf
σi = (po - pv) / (ρVo2 /2)
161 = [(25 × 144 in2/ft2) - 37)] / [ 1.94 Vo2/2]
Vo = 4.78 fps
Q = Vo Ao = Vo (π/4) Do2 = 4.78 (0.7854) (2)2 = 15 cfs.