Question 6.16: Water, ρ = 1.94 slugs/ft^3 and ν = 0.000011 ft^2/s, is pumpe...

Water, ρ = 1.94 slugs/ft^3 and ν = 0.000011 ft^2/s, is pumped between two reservoirs at 0.2 ft^3/s through 400 ft of 2-in-diameter pipe and several minor losses, as shown in Fig. E6.16. The roughness ratio is ε/d = 0.001. Compute the pump horsepower required.

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Write the steady flow energy equation between sections 1 and 2, the two reservoir surfaces:

\frac{p_1}{\rho g} + \frac{V^2_1}{2g} + z_1 = \left(\frac{p_2}{\rho g} + \frac{V^2_2}{2g} + z_2\right) + h_f + \sum{h_m} – h_p

where h_p is the head increase across the pump. But since p_1 = p_2 and V_1 = V_2 \approx 0, solve for the pump head:

h_p = z_2 – z_1 + h_f + \sum{h_m} = 120  ft – 20  ft + \frac{V^2}{2g}\left(\frac{fL}{d} + \sum{K}\right)                             (1)

Now with the flow rate known, calculate

V = \frac{Q}{A} = \frac{0.2  ft^3/s}{\frac{1}{4} \pi (\frac{2}{12}  ft)^2} = 9.17  ft/s

Now list and sum the minor loss coefficients:

Loss K
Sharp entrance (Fig. 6.21) 0.5
Open globe valve (2 in, Table 6.5) 6.9
12-in bend (Fig. 6.20) 0.25
Regular 90° elbow (Table 6.5) 0.95
Half-closed gate valve (from Fig. 6.18b) 2.7
Sharp exit (Fig. 6.21) 1.0
Σ K = 12.3
Table 6.5 Nominal diameter, in
Screwed Flanged
\frac{1}{2} 1 2 4 1 2 4 8 20
Valves (fully open):
Globe 14 8.2 6.9 5.7 13 8.5 6.0 5.8 5.5
Gate 0.30 0.24 0.16 0.11 0.8 0.35 0.16 0.07 0.03
Swing check 5.1 2.9 2.1 2.0 2.0 2.0 2.0 2.0 2.0
Angle 9.0 4.7 2.0 1.0 4.5 2.4 2.0 2.0 2.0
Elbows:
45° regular 0.39 0.32 0.30 0.29
45° long radius 0.21 0.20 0.19 0.16 0.14
90° regular 2.0 1.5 0.95 0.64 0.50 0.39 0.30 0.26 0.21
90° long radius 1.0 0.72 0.41 0.23 0.40 0.30 0.19 0.15 0.10
180° regular 2.0 1.5 0.95 0.64 0.41 0.35 0.30 0.25 0.20
180° long radius 0.40 0.30 0.21 0.15 0.10
Tees:
Line flow 0.90 0.90 0.90 0.90 0.24 0.19 0.14 0.10 0.07
Branch flow 2.4 1.8 1.4 1.1 1.0 0.8 0.64 0.58 0.41

Calculate the Reynolds number and pipe friction factor:

Re_d = \frac{Vd}{\nu} = \frac{9.17(\frac{2}{12})}{0.000011} = 139,000

For ε/d = 0.001, from the Moody chart read f = 0.0216. Substitute into Eq. (1):

h_p = 100  ft + \frac{(9.17  ft/s)^2}{2(32.2  ft/s^2)} \left[\frac{0.0216(400)}{\frac{2}{12}} + 12.3\right] = 100  ft + 84  ft = 184  ft            pump head

The pump must provide a power to the water of

P = \rho gQh_p = [1.94(32.2)  lbf/ft^3] (0.2  ft^3/s)(184  ft) = 2300  ft \cdot lbf/s

The conversion factor is 1 hp = 550 ft · lbf/s. Therefore

P = \frac{2300}{550} = 4.2 hp

Allowing for an efficiency of 70 to 80 percent, a pump is needed with an input of about 6 hp.

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