Use orifice equation: Q = K Ao (2g Δh)1/2
Assume d, find K from Fig. 5-21, and calculate Q. Repeat for another d.
First trial: d = 2 ft
d / D = 2 / 4 = 0.5
Δh = Δp/γ = (2000 lbs/ft2)/(62.4 lbs/ft3) = 32.05 ft
(2 g Δh)1/2 = (2 × 32.17 × 32.05) 1/2 = 45.41
For T= 60oF: ν = 1.217 × 10-5 ft2/s
(2 g Δh)1/2 d/ν = 45.41 × 2 / (1.217 × 10-5) = 7.46 × 106
From Fig. 5-21: K = 0.63
Q = 0.63 (π/4) (2)2 × 45.41 = 90 cfs [Discharge is too low; orifice too small]
Second trial: d = 2.5; d / D = 0.625.
Δh = Δp/γ = (2000 lbs/ft2)/(62.4 lbs/ft3) = 32.05 ft
(2 g Δh)1/2 = (2 × 32.17 × 32.05) 1/2 = 45.41
For T= 60oF: ν = 1.217 × 10-5 ft2/s
(2 g Δh)1/2 d/ν = 45.41 × 2.5 / (1.217 × 10-5) = 9.33 × 106
From Fig. 5-21: K = 0.66
Q = 0.66 (π/4) (2.5)2 × 45.41 =147 cfs [Discharge is too large; orifice too big]
Third trial: d = 2.1; d / D = 0.525.
Δh = Δp/γ = (2000 lbs/ft2)/(62.4 lbs/ft3) = 32.05 ft
(2 g Δh)1/2 = (2 × 32.17 × 32.05) 1/2 = 45.41
For T= 60oF: ν = 1.217 × 10-5 ft2/s
(2 g Δh)1/2 d/ν = 45.41 × 2.1 / (1.217 × 10-5) = 7.83 × 106
From Fig. 5-21: K = 0.63
Q = 0.63 (π/4) (2.1)2 × 45.41 = 99 cfs [Discharge is ok now; orifice diameter ok]
ks / D = 0.004 ft / 1 ft = 0.004
Assume very high Reynolds number. Estimate f from Moody diagram: f = 0.028.
Velocity head is lost in the free jet: KE = 1
Write the energy equation between the reservoir water surface elevation and [the elevation of the] free jet.
100 - 64 = [f (L/D) + Ke + Kb + KE] [V2/(2g)]
36 = [ 0.028 × (100/1) + 0.12 + 0.35 + 1 ] [V2/(2 × 32.17)]
36 = 4.27 (V2/64.34)
V = 23.29 fps.
V2/(2g) = (23.29)2/(2 × 32.17) = 8.43 ft.
The velocity head is 8.43 ft.
A = (π/4) D2 = (3.1416/4) (1)2 = 0.7854 ft2
Q = 23.29 × 0.7854 = 18.29 cfs.
For T = 60oF : ν = 1.217 × 10-5 ft2/s
Calculate Reynolds number: Re = VD/ν = 23.29 × 1 / (1.217 × 10-5) = 1.9 × 106
From Fig. 5-4: f = 0.028. [Assumed value is OK].
The point of maximum pressure pmax is right above (upstream) of the 90o bend.
Write the energy equation between a point immediately upstream of the bend (max) and a point (2) at the exit.
The velocity heads are the same, so they cancel.
(pmax/γ) + zmax = (p2/γ) + z2 + Σ hL
p2/γ = 0
(pmax/γ) + 44 = 0 + 64 + [f (L/D) + Kb ][V2/(2g)]
(pmax/γ) + 44 = 0 + 64 + [0.028 (28/1) + 0.35](8.43)
pmax/γ = 20 + 9.56 = 29.56
pmax = γ (29.56) = 1845 lb/ft2
Or, alternatively, write the energy equation between the reservoir water surface elevation (1) and a point immediately upstream of the bend (max)
The velocity heads are the same, so they cancel.
(p1/γ) + z1 = (pmax/γ) + zmax + Σ hL
p1/γ = 0
0 + 100 = (pmax/γ) + 44 + [ f (L/D) + Ke + 1] [V2/(2g)]
56 = (pmax/γ) + [ 0.028 (72/1) + 0.12 + 1] [8.43]
56 = (pmax/γ) + 26.43
pmax/γ = 29.57 ft.
pmax = 1845 lb/ft2
Immediately upstream of the pipe entrance, the pressure head is 5 ft and the velocity head is 0.
Immediately downstream of the pipe entrance, the velocity head is 8.43 ft, and the drop in pressure head is 8.43(1 + 0.12)
Therefore, the point of minimum pressure is immediately downstream of the pipe entrance.
pmin = 62.4 × [5 - 8.43(1 + 0.12)] = -277 lb/ft2.