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Properties of Matter question

2019 · 8 Apr · Shift 1 · Q70
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Properties of Matter question

2019 · 8 Apr · Shift 1 · Q70

JEE MainPhysicsProperties of MatterMCQ+4 / −1
A boy's catapult is made of rubber cord which is 42 cm long, with 6 mm diameter of cross-section and of negligible mass. The boy keeps a stone weighing 0.02kg on it and stretches the cord by 20 cm by applying a constant force. When released, the stone flies off with a velocity of 20 ms–1. Neglect the change in the area of cross-section of the cord while stretched. The Young's modulus of rubber is closest to:
  1. A
    104 Nm–2
  2. B
    106 Nm–2
  3. C
    108 Nm–2
  4. D
    103 Nm–2
View written solutionFree

Correct answer: B

  1. Given data
  • Original length of rubber cord: L=42 cm=0.42 mL = 42\text{ cm} = 0.42\text{ m}L=42 cm=0.42 m
  • Extension: x=20 cm=0.20 mx = 20\text{ cm} = 0.20\text{ m}x=20 cm=0.20 m
  • Diameter of cord: d=6 mm=6×10−3 md = 6\text{ mm} = 6 \times 10^{-3}\text{ m}d=6 mm=6×10−3 m
  • Radius: r=3×10−3 mr = 3 \times 10^{-3}\text{ m}r=3×10−3 m
  • Mass of stone: m=0.02 kgm = 0.02\text{ kg}m=0.02 kg
  • Speed of stone on release: v=20 m s−1v = 20\text{ m s}^{-1}v=20 m s−1

We assume the elastic potential energy stored in the stretched rubber becomes the kinetic energy of the stone.


  1. Elastic energy stored in the cord

Since the boy stretches the cord by applying a constant force, the force-extension graph is a straight line from 000 to the final force FFF.

Hence, elastic energy stored is

U=12FxU = \frac{1}{2}FxU=21​Fx

This becomes kinetic energy of the stone:

12Fx=12mv2\frac{1}{2}Fx = \frac{1}{2}mv^221​Fx=21​mv2

So,

Fx=mv2Fx = mv^2Fx=mv2

F=mv2xF = \frac{mv^2}{x}F=xmv2​

Substitute values:

F=0.02×(20)20.20=0.02×4000.20=820×10=40 NF = \frac{0.02 \times (20)^2}{0.20} = \frac{0.02 \times 400}{0.20} = \frac{8}{20} \times 10 = 40\text{ N}F=0.200.02×(20)2​=0.200.02×400​=208​×10=40 N

So the final stretching force is

F=40 NF = 40\text{ N}F=40 N


  1. Use Young's modulus formula

Young's modulus is

Y=stressstrain=F/Ax/L=FLAxY = \frac{\text{stress}}{\text{strain}} = \frac{F/A}{x/L} = \frac{FL}{Ax}Y=strainstress​=x/LF/A​=AxFL​

Cross-sectional area:

A=πr2=π(3×10−3)2=9π×10−6 m2A = \pi r^2 = \pi (3 \times 10^{-3})^2 = 9\pi \times 10^{-6}\text{ m}^2A=πr2=π(3×10−3)2=9π×10−6 m2

Now,

Y=40×0.42(9π×10−6)×0.20Y = \frac{40 \times 0.42}{(9\pi \times 10^{-6}) \times 0.20}Y=(9π×10−6)×0.2040×0.42​

Y=16.81.8π×10−6Y = \frac{16.8}{1.8\pi \times 10^{-6}}Y=1.8π×10−616.8​

Using π≈3.14\pi \approx 3.14π≈3.14,

Y≈16.85.652×10−6Y \approx \frac{16.8}{5.652 \times 10^{-6}}Y≈5.652×10−616.8​

Y≈2.97×106 N m−2Y \approx 2.97 \times 10^6\text{ N m}^{-2}Y≈2.97×106 N m−2

Thus,

Y≈3×106 N m−2Y \approx 3 \times 10^6\text{ N m}^{-2}Y≈3×106 N m−2


  1. Choose the closest option

The value is of the order of

106 N m−210^6\text{ N m}^{-2}106 N m−2

So the closest option is:

Option B: 106 N m−210^6\text{ N m}^{-2}106 N m−2


  1. Verification with stored answer

Stored correct answer: B

Our derived answer: B

So they agree.

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