2019 A/L Physics Past Paper · Question 39 (English Medium)

Flow rate from the height difference of two vertical tubes

As shown in the figure, an incompressible liquid flows steadily through a horizontal pipe. Two narrow vertical tubes are fixed at two places on the horizontal pipe where the cross-sectional areas are AA and 2A2A. If the height difference of the liquid columns in the two vertical tubes is hh, flow rate of the liquid through the pipe is

  1. (1) A2ghA\sqrt{2gh}
  2. (2) A6ghA\sqrt{6gh}
  3. (3) A3gh2A\sqrt{\frac{3gh}{2}}
  4. (4) 2Agh32A\sqrt{\frac{gh}{3}}
  5. (5) 2A2gh32A\sqrt{\frac{2gh}{3}}
Answer and explanation

Answer: (5) 2A2gh32A\sqrt{\frac{2gh}{3}}

What the question asks

The columns in the two tubes differ in height by hh.

We want the flow rate QQ in terms of AA, gg and hh.

Relevant theory

Volume of fluid entering the tube through area A1A_1.

Since the flow is continuous, the volume of fluid flowing past the cross section A2A_2 per unit is the same.

On any point along the same streamline of a steady flow of an incompressible fluid of negligible viscosity, the sum of the pressure, the potential energy per unit volume and the kinetic energy per unit volume is a constant.

Required equations

Q=Av1=2Av2Q = Av_1 = 2Av_2

p1+12ρv12=p2+12ρv22p_1 + \frac{1}{2}\rho v_1^2 = p_2 + \frac{1}{2}\rho v_2^2

p2−p1=ρghp_2 - p_1 = \rho g h

Reasoning and calculation

The letters:

v1v_1, p1p_1: speed and pressure in the narrow part, area AA.

v2v_2, p2p_2: speed and pressure in the wide part, area 2A2A.

ρ\rho: the density of the liquid.

hh: the height difference of the columns.

QQ: the volume of liquid that flows each second.

The same liquid passes both parts each second.

The wide part is twice as big, so v2=v12v_2 = \dfrac{v_1}{2}.

The narrow part is faster. So its pressure is lower, and its column is lower.

The pressure difference is the weight of the height hh of liquid:

p2−p1=ρghp_2 - p_1 = \rho g h

ρgh=12ρ(v12−v124)=38ρv12\rho g h = \frac{1}{2}\rho\left(v_1^2 - \frac{v_1^2}{4}\right) = \frac{3}{8}\rho v_1^2

v1=8gh3v_1 = \sqrt{\frac{8gh}{3}}

Q=A8gh3=2A2gh3Q = A\sqrt{\frac{8gh}{3}} = 2A\sqrt{\frac{2gh}{3}}

Reading the options

The answer has the form 2A2gh32A\sqrt{\frac{2gh}{3}}.

That is option (5).

Checks

Check the units.

AghA\sqrt{gh} has the dimensions L2⋅LT−1=L3T−1L^2 \cdot LT^{-1} = L^3T^{-1}.

That is a volume each second, a flow rate. ✓

Check the limit.

If h=0h = 0, then Q=0Q = 0 ✓.

No flow, no pressure difference.

If the two parts were equal (2A→A2A \to A), the speeds would be equal and hh would be 0.

The height difference comes from the change in area.

Conclusion

Q=2A2gh3Q = 2A\sqrt{\frac{2gh}{3}}

38v12=gh\frac{3}{8}v_1^2 = gh

Q=Av1=2A2gh3Q = Av_1 = 2A\sqrt{\frac{2gh}{3}}

So the answer is option (5).

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