MCQEasyJEE 2025Moment of Inertia & Radius of Gyration

JEE Physics 2025 Question with Solution

A cord of negligible mass is wound around the rim of a wheel supported by spokes with negligible mass. The mass of the wheel is 10kg10 \, \text{kg} and radius is 10cm10 \, \text{cm} and it can freely rotate without any friction. Initially the wheel is at rest. If a steady pull of 20N20 \, \text{N} is applied on the cord, the angular velocity of the wheel, after the cord is unwound by 1m1 \, \text{m}, will be:

  • A

    20rad/s20 \, \text{rad/s}

  • B

    30rad/s30 \, \text{rad/s}

  • C

    10rad/s10 \, \text{rad/s}

  • D

    0rad/s0 \, \text{rad/s}

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: Mass of the wheel = 10kg10 \, \text{kg}, radius = 0.1m0.1 \, \text{m}, applied force = 20N20 \, \text{N}, unwound length = 1m1 \, \text{m}. The wheel starts from rest and the spokes have negligible mass, so the wheel is treated as a ring.

Find: The angular velocity of the wheel after the cord is unwound by 1m1 \, \text{m}.

Using the work-energy theorem for rotational motion, the work done by the steady pull becomes rotational kinetic energy.

The work done by the force is

Wf=Fd=20×1=20JW_f = F \cdot d = 20 \times 1 = 20 \, \text{J}

This equals the change in kinetic energy of the wheel:

KE=12Iω2KE = \frac{1}{2} I \omega^2

For a ring,

I=MR2I = MR^2

Substituting the given values:

I=10×(0.1)2=0.1kg m2I = 10 \times (0.1)^2 = 0.1 \, \text{kg m}^2

Now equating work done to rotational kinetic energy:

20=12×0.1×ω220 = \frac{1}{2} \times 0.1 \times \omega^2 ω2=400\omega^2 = 400 ω=20rad/s\omega = 20 \, \text{rad/s}

Therefore, the angular velocity of the wheel is 20rad/s20 \, \text{rad/s}. The correct option is A.

Detailed Work-Energy Approach

Given:

  • Mass of the wheel, M=10kgM = 10 \, \text{kg}
  • Radius of the wheel, R=10cm=0.1mR = 10 \, \text{cm} = 0.1 \, \text{m}
  • Applied force, F=20NF = 20 \, \text{N}
  • Length of unwound cord, L=1mL = 1 \, \text{m}
  • Initial angular velocity, ωi=0rad/s\omega_i = 0 \, \text{rad/s}

Find: Final angular velocity ωf\omega_f.

This solution uses the work-energy theorem for rotational motion.

  1. Since the spokes have negligible mass, the wheel is treated as a ring. Hence its moment of inertia is
I=MR2I = MR^2

Substituting values,

I=(10kg)×(0.1m)2=10×0.01=0.1kgm2I = (10 \, \text{kg}) \times (0.1 \, \text{m})^2 = 10 \times 0.01 = 0.1 \, \text{kg} \cdot \text{m}^2
  1. The work done by the applied force over the unwound length is
W=F×LW = F \times L

So,

W=(20N)×(1m)=20JW = (20 \, \text{N}) \times (1 \, \text{m}) = 20 \, \text{J}
  1. Apply the work-energy theorem:
W=KErot, finalKErot, initialW = KE_{\text{rot, final}} - KE_{\text{rot, initial}}

Since the wheel starts from rest, initial rotational kinetic energy is zero. Therefore,

W=12Iωf2W = \frac{1}{2} I \omega_f^2

Substituting the calculated values,

20=12(0.1)ωf220 = \frac{1}{2} (0.1) \omega_f^2 ωf2=2×200.1=400.1=400\omega_f^2 = \frac{2 \times 20}{0.1} = \frac{40}{0.1} = 400 ωf=400=20rad/s\omega_f = \sqrt{400} = 20 \, \text{rad/s}

Therefore, the angular velocity of the wheel after the cord is unwound by 1m1 \, \text{m} is 20rad/s20 \, \text{rad/s}.

Common mistakes

  • Using the moment of inertia of a solid disc instead of a ring is incorrect here because the spokes have negligible mass, so the mass is effectively concentrated at the rim. Use I=MR2I = MR^2, not I=12MR2I = \frac{1}{2}MR^2.

  • Treating the pulled length as arc length without using work-energy can lead to unnecessary confusion. The solution directly uses the work done by the force, W=FdW = Fd, and sets it equal to rotational kinetic energy.

  • Forgetting that the wheel starts from rest is wrong because then an extra initial kinetic energy term may be introduced incorrectly. Here ωi=0\omega_i = 0, so the initial rotational kinetic energy is zero.

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