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Air flows at the rate of 1.5 m3/s through a horizontal pipe with a gradually reducing cross-section as shown in the figure. The two cross-sections of the pipe have diameters of 400 mm and 200 mm. Take the air density as 1.2 kg/m3 and assume inviscid incompressible flow. The change in pressure (p2 − p1) (in kPa) between sections 1 and 2 is

Pipe carrying air flow of 1.5 cubic metres per second from left to right, narrowing from section 1 of diameter 400 mm to section 2 of diameter 200 mm

  • A.−1.28
  • B.2.56
  • C.−2.13
  • D.1.28

Answer: A

The pressure change is -1.28 kPa.

Continuity gives the velocities from Q = 1.5 m3/s:

\[ \begin{aligned} V_{1} &= \frac{1.5}{\pi(0.2)^{2}} = 11.94\ \text{m/s} \\ V_{2} &= \frac{1.5}{\pi(0.1)^{2}} = 47.75\ \text{m/s} \end{aligned} \]

Bernoulli's equation for a horizontal pipe then gives

\[ \begin{aligned} p_{2} - p_{1} &= \frac{\rho}{2}\left(V_{1}^{2} - V_{2}^{2}\right) \\ &= 0.6\,(142.5 - 2280.0) \\ &= -1282\ \text{Pa} \approx -1.28\ \text{kPa} \end{aligned} \]

The pressure falls as the flow speeds up in the narrower section, so the change is negative; +1.28 has the sign reversed. 2.56 doubles the result by dropping the 1/2, and -2.13 does not follow from these data.

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