2021 A/L Physics Past Paper · Question 49 (English Medium)

Force of the water on the sloping wall of a flask

The figure shows a vertical cross-section of a conical flask filled with water. The height of the water level in the flask is 0.25 m0.25\ \text{m} and its circular base has an internal diameter of 0.20 m0.20\ \text{m}. The volume of water in the flask is 2.5×10−3 m32.5 \times 10^{-3}\ \text{m}^3. What is the magnitude of the total force exerted by the water on the inclined surface of the flask? Density of water =103 kg m−3= 10^3\ \text{kg m}^{-3}. (Take π=3\pi = 3.)

  1. (1) 10 N10\ \text{N}
  2. (2) 20 N20\ \text{N}
  3. (3) 30 N30\ \text{N}
  4. (4) 40 N40\ \text{N}
  5. (5) 50 N50\ \text{N}
Answer and explanation

Answer: (5) 50 N50\ \text{N}

Given information

What we know:

Height of the water: H=0.25 mH = 0.25\ \text{m}.

Diameter of the base: 0.20 m0.20\ \text{m}, so the radius is 0.10 m0.10\ \text{m}.

Volume of the water: V=2.5×10−3 m3V = 2.5 \times 10^{-3}\ \text{m}^3.

Density of water: ρ=103 kg m−3\rho = 10^3\ \text{kg m}^{-3}. Take π=3\pi = 3.

The paper does not give gg. We take g=10 m s−2g = 10\ \text{m s}^{-2}, as the marking scheme does.

What the question asks

Find the force that the water exerts on the sloping surface of the flask.

The plan has three steps.

First, find the force of the water on the base.

Then find the weight of the water.

The sloping wall must carry the difference.

Relevant theory

As pressure is the force acting normally on a unit area,

When the objects interact (collide), they exert equal and oppsite forces on one another.

Required equations

p=Hρgp = H\rho g

Fbase=pAF_{\text{base}} = pA

W=ρVgW = \rho V g

Fbase=W+FwallF_{\text{base}} = W + F_{\text{wall}}

Applying it to this question

The water is at rest.

The base pushes the water up.

The weight pulls it down. The sloping wall pushes it down and inwards.

The sideways pushes of the wall cancel all round the flask. Only the vertical part is left.

0.030.03

A=πr2=3×0.102A = \pi r^2 = 3 \times 0.10^2

25002500

p=Hρg=0.25×1000×10p = H\rho g = 0.25 \times 1000 \times 10

7575

Fbase=pA=2500×0.03F_{\text{base}} = pA = 2500 \times 0.03

2525

W=ρVg=1000×2.5×10−3×10W = \rho V g = 1000 \times 2.5 \times 10^{-3} \times 10

5050

Fwall=Fbase−W=75−25F_{\text{wall}} = F_{\text{base}} - W = 75 - 25

All quantities are in SI units.

Pressure in Pa=N m−2\text{Pa} = \text{N m}^{-2}, area in m2\text{m}^2, so the force is in newtons.

Reasoning and calculation

The sloping wall pushes the water with 50 N50\ \text{N}.

The water pushes the wall with an equal and opposite force.

So the water exerts 50 N50\ \text{N} on the inclined surface.

The answer is (5).

Checks

H∗rho∗g∗3∗r∗r−rho∗V∗gH * rho * g * 3 * r * r - rho * V * g

Does it make sense?

The flask narrows upwards. So it holds less water than a straight column of height 0.25 m0.25\ \text{m} over the base would. That column would weigh 75 N75\ \text{N}.

The base feels 75 N75\ \text{N}, three times the weight of the water. The sloping wall carries the extra 50 N50\ \text{N}.

Conclusion

Fwall=HρgA−ρVg=75−25=50 NF_{\text{wall}} = H\rho g A - \rho V g = 75 - 25 = 50\ \text{N}

The force on the base is pA=2500×0.03=75 NpA = 2500 \times 0.03 = 75\ \text{N}.

The water weighs 25 N25\ \text{N}.

So the sloping wall takes 75−25=50 N75 - 25 = 50\ \text{N}. The answer is (5).

In a flask that is wider at the bottom, the base force can be larger than the weight of the water.

Find the base force from the pressure. Subtract the weight. The sloping wall carries the rest.

Exam tip

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