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Inclined smooth pipe with wall shear limit

Short answer

The flow is turbulent. Equating wall shear stress to the turbulent friction relation yields V ≈ 6.96 m/s, giving Q = 54.7 L/s. Using the force balance along the pipe, the maximum inlet gauge pressure is about 692 kPa.

A straight smooth pipe 100 mm diameter and 60 m long is inclined at 10° to the horizontal. A liquid of relative density 0.9 and kinematic viscosity 120 mm²/s is to be pumped through it into a reservoir at the upper end where the gauge pressure is 120 kPa. The pipe friction factor f is given by 64/Re for laminar flow and by 0.32 Re−1/40.32\,Re^{-1/4} for turbulent flow when Re < 10510^5. Determine (a) the maximum pressure at the lower, inlet, end of the pipe if the mean shear stress at the pipe wall is not to exceed 200 Pa; (b) the corresponding rate of flow.

Data. D=0.1D = 0.1 m, L=60L = 60 m, inclination 10°, ρ=900\rho = 900 kg/m³ (R.D. 0.9), ν=120\nu = 120 mm²/s =1.2×10−4= 1.2\times10^{-4} m²/s, outlet gauge pressure p2=120p_2 = 120 kPa, maximum mean wall shear τ0=200\tau_0 = 200 Pa.

Which flow regime?

Mean wall shear in terms of ff: τ0=fρV28\tau_0 = \dfrac{f\rho V^2}{8}.

  • If laminar: τ0=8μVD\tau_0 = \dfrac{8\mu V}{D}, i.e. V=τ0D8μ=200(0.1)8(900)(1.2×10−4)=23.15V = \dfrac{\tau_0 D}{8\mu} = \dfrac{200(0.1)}{8(900)(1.2\times10^{-4})} = 23.15 m/s, giving Re=19290Re = 19290, which is not laminar. So the flow is turbulent.
  • Turbulent: f=0.32 Re−1/4f = 0.32\,Re^{-1/4} (valid since Re<105Re < 10^5).

(b) Flow rate

τ0=ρV28(0.32)(νVD)1/4=0.04 ρ(νD)1/4V7/4\tau_0 = \frac{\rho V^2}{8}(0.32)\left(\frac{\nu}{VD}\right)^{1/4} = 0.04\,\rho\left(\frac{\nu}{D}\right)^{1/4} V^{7/4} 200=0.04(900)(1.2×10−40.1)1/4V1.75=6.700 V1.75200 = 0.04(900)\left(\frac{1.2\times10^{-4}}{0.1}\right)^{1/4} V^{1.75} = 6.700\,V^{1.75} V=(2006.700)1/1.75=6.963 m/sV = \left(\frac{200}{6.700}\right)^{1/1.75} = 6.963\ \text{m/s}

Check: Re=6.963(0.1)1.2×10−4=5803<105Re = \dfrac{6.963(0.1)}{1.2\times10^{-4}} = 5803 < 10^5, so the formula applies; f=0.32Re−1/4=0.03666f = 0.32Re^{-1/4} = 0.03666 and fρV28=200.0\dfrac{f\rho V^2}{8} = 200.0 Pa.

Q=π4D2V=π4(0.1)2(6.963)=0.05469 m3/s=54.69 l/sQ = \frac{\pi}{4}D^2V = \frac{\pi}{4}(0.1)^2(6.963) = 0.05469\ \text{m}^3/\text{s} = 54.69\ \text{l/s}

(a) Maximum inlet pressure

Force balance on the liquid in the pipe along the incline (steady, uniform flow):

(p1−p2)πD24=τ0 πDL+ρg πD24Lsin⁡θ(p_1 - p_2)\frac{\pi D^2}{4} = \tau_0\,\pi D L + \rho g\,\frac{\pi D^2}{4}L\sin\theta p1−p2=4τ0LD+ρgLsin⁡θ=4(200)(60)0.1+900(9.81)(60)sin⁡10∘p_1 - p_2 = \frac{4\tau_0L}{D} + \rho g L\sin\theta = \frac{4(200)(60)}{0.1} + 900(9.81)(60)\sin10^\circ p1−p2=480000+91988=571988 Pap_1 - p_2 = 480000 + 91988 = 571988\ \text{Pa} p1=120 000+480000+91988=691988 Pa≈692 kPa (gauge)p_1 = 120\,000 + 480000 + 91988 = 691988\ \text{Pa} \approx 692\ \text{kPa (gauge)}

Answer: (a) p1,max≈692p_{1,max} \approx 692 kPa gauge; (b) Q=54.7Q = 54.7 l/s (V=6.96V = 6.96 m/s).

✓ Answer checked by Claude Sonnet 5.5

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