Skip to main content

Duration of flow after pump stops

Short answer

With rigid-column theory, the deceleration equation is integrated from initial flow to zero. The flow into the tank continues for 2.62 s after power failure.

A pump draws water from a reservoir and delivers it through a pipe 150 mm diameter, 90 m long, to a tank in which the free surface level is 8 m higher than that in the reservoir. The flow rate is steady at 0.05 m³/s until a power failure causes the pump to stop. Neglecting minor losses in the pipe and in the pump and assuming that the pump stops instantaneously, determine for how long flow into the tank continues after the power failure. The friction factor f may be taken as constant at 0.028 and elastic effects in the water or pipe material may be disregarded.

Data. D=0.15D = 0.15 m, L=90L = 90 m, static lift Hs=8H_s = 8 m, f=0.028f = 0.028, steady Q0=0.05Q_0 = 0.05 m³/s. The pump stops instantaneously; minor losses and elasticity are neglected, so the water column decelerates as a rigid body under the static head (back-pressure) and friction.

Constants

A=π4(0.15)2=0.01767 m2,I=LA=900.01767=5093.0 m−1A = \frac{\pi}{4}(0.15)^2 = 0.01767\ \text{m}^2,\qquad I = \frac{L}{A} = \frac{90}{0.01767} = 5093.0\ \text{m}^{-1} r=8fLπ2gD5=8(0.028)(90)π2(9.81)(0.15)5=2742.0 s2/m5(steady friction head rQ02=6.85 m)r = \frac{8fL}{\pi^2gD^5} = \frac{8(0.028)(90)}{\pi^2(9.81)(0.15)^5} = 2742.0\ \text{s}^2/\text{m}^5 \quad(\text{steady friction head } rQ_0^2 = 6.85\ \text{m})

Equation of motion

LgAdQdt=−(Hs+rQ2)  ⇒  dt=−IgdQHs+rQ2\frac{L}{gA}\frac{dQ}{dt} = -\left(H_s + rQ^2\right) \;\Rightarrow\; dt = -\frac{I}{g}\frac{dQ}{H_s + rQ^2}

The flow into the tank stops when Q=0Q = 0. Integrating from Q0Q_0 to 0:

t=Ig∫0Q0dQHs+rQ2=IgHsrtan⁡−1(Q0rHs)t = \frac{I}{g}\int_0^{Q_0}\frac{dQ}{H_s + rQ^2} = \frac{I}{g\sqrt{H_sr}}\tan^{-1}\left(Q_0\sqrt{\frac{r}{H_s}}\right) Q0rHs=0.052742.08=0.9257,tan⁡−1(0.9257)=0.7468 radQ_0\sqrt{\frac{r}{H_s}} = 0.05\sqrt{\frac{2742.0}{8}} = 0.9257,\qquad \tan^{-1}(0.9257) = 0.7468\ \text{rad} t=5093.09.818(2742.0)(0.7468)=0.74680.28528=2.62 st = \frac{5093.0}{9.81\sqrt{8(2742.0)}}(0.7468) = \frac{0.7468}{0.28528} = 2.62\ \text{s}

Answer: The flow into the tank continues for about 2.622.62 s (about 2.6 s) after the power failure.

✓ Answer checked by Claude Opus 5.5 (high effort)

All Hydraulics chapter 4 questions →