What should the reservoir level h be to maintain a flow of 0.01 m^3/s through the commercial steel annulus 30 m long shown in Fig. E6.14? Neglect entrance effects and take ρ = 1000 kg/m^3 and ν = 1.02 × 10^{-6} m^2/s for water.
What should the reservoir level h be to maintain a flow of 0.01 m^3/s through the commercial steel annulus 30 m long shown in Fig. E6.14? Neglect entrance effects and take ρ = 1000 kg/m^3 and ν = 1.02 × 10^{-6} m^2/s for water.
• Assumptions: Fully developed annulus flow, minor losses neglected.
• Approach: Determine the Reynolds number, then find f and h_f and thence h.
• Property values: Given ρ = 1000 kg/m^3 and ν = 1.02E-6 m^2/s.
• Solution step 1: Calculate the velocity, hydraulic diameter, and Reynolds number:
V = \frac{Q}{A} = \frac{0.01 m^3/s}{\pi [(0.05 m)^2 (0.03 m)^2]} = 1.99 \frac{m}{s} D_h = 2(a – b) = 2(0.05 m – 0.03 m) = 0.04 mRe_{D_h} = \frac{VD_h}{\nu} = \frac{(1.99 m/s)(0.04 m)}{1.02E-6 m^2/s} = 78,000 (turbulent flow)
• Solution step 2: Apply the steady flow energy equation between sections 1 and 2:
\frac{p_1}{\rho g} + \frac{\alpha_1 V_1^2}{2g} + z_1 = \frac{p_2}{\rho g} + \frac{\alpha_2 V_2^2}{2g} + z_2 + h_for h = \frac{\alpha_2 V_2^2}{2g} + h_f = \frac{V_2^2}{2g} \left(\alpha_2 + f\frac{L}{D_h}\right) (1)
Note that z_1 = h. For turbulent flow, from Eq. (3.43c), we estimate \alpha_2 ≈ 1.03
\beta = \frac{(1 + m)^2(2 + m)^2}{2(1 + 2m)(2 + 2m)} (3.43c)
• Solution step 3: Determine the roughness ratio and the friction factor. From Table 6.1, for (new) commercial steel pipe, ε = 0.046 mm. Then
\frac{\epsilon}{D_h} = \frac{0.046 mm}{40 mm} = 0.00115Table 6.1: ε | ||||
Material | Condition | ft | mm | Uncertainty, % |
Steel | Sheet metal, new | 0.0002 | 0.05 | ±60 |
Stainless, new | 7E-06 | 0.002 | ±50 | |
Commercial, new | 0.0002 | 0.046 | ±30 | |
Riveted | 0.01 | 3 | ±70 | |
Rusted | 0.007 | 2 | ±50 | |
Iron | Cast, new | 0.0009 | 0.26 | ±50 |
Wrought, new | 0.0002 | 0.046 | ±20 | |
Galvanized, new | 0.0005 | 0.15 | ±40 | |
Asphalted cast | 0.0004 | 0.12 | ±50 | |
Brass | Drawn, new | 7E-06 | 0.002 | ±50 |
Plastic | Drawn tubing | 5E-06 | 0.0015 | ±60 |
Glass | – | Smooth | Smooth | |
Concrete | Smoothed | 0.0001 | 0.04 | ±60 |
Rough | 0.007 | 2 | ±50 | |
Rubber | Smoothed | 3E-05 | 0.01 | ±60 |
Wood | Stave | 0.0016 | 0.5 | ±40 |
For a reasonable estimate, use Re_{D_h} to estimate the friction factor from Eq. (6.48):
\frac{1}{\sqrt{f}} = -2.0 \log_{10} \left(\frac{0.00115}{3.7} + \frac{2.51}{78,000 \sqrt{f}}\right) solve for f ≈ 0.0232
For slightly better accuracy, we could use D_{eff} = D_h / \zeta. From Table 6.3, for b/a = 3/5, 1/ζ = 0.67. Then D_{eff} = 0.67(40 mm) = 26.8 mm, whence Re_{D_{eff}} = 52,300, \epsilon /D_{eff} = 0.00172, and f_{eff} ≈ 0.0257. Using the latter estimate, we find the required reservoir level from Eq. (1):
h = \frac{V^2_2}{2g} \left(\alpha_2 + f_{eff}\frac{L}{D_h}\right) = \frac{(1.99 m/s)^2}{2(9.81 m/s)^2} \left[1.03 + 0.0257 \frac{30 m}{0.04 m}\right] = 4.1 mTable 6.3 | Laminar Friction Factors for a Concentric Annulus |
|
b/a | f Re_{D_h} | D_{eff}/D_h = 1/ \zeta |
0.0 | 64.0 | 1.000 |
0.00001 | 70.09 | 0.913 |
0.0001 | 71.78 | 0.892 |
0.001 | 74.68 | 0.857 |
0.01 | 80.11 | 0.799 |
0.05 | 86.27 | 0.742 |
0.1 | 89.37 | 0.716 |
0.2 | 92.35 | 0.693 |
0.4 | 94.71 | 0.676 |
0.6 | 95.59 | 0.670 |
0.8 | 95.92 | 0.667 |
1.0 | 96.0 | 0.667 |
• Comments: Note that we do not replace D_h by D_{eff} in the head loss term fL/D_h, which comes from a momentum balance and requires hydraulic diameter. If we used the simpler friction estimate, f ≈ 0.0232, we would obtain h ≈ 3.72 m, or about 9 percent lower.