MCQEasyJEE 2025Torque & Angular Momentum

JEE Physics 2025 Question with Solution

A circular disk of radius RR meter and mass MM kg is rotating around the axis perpendicular to the disk. An external torque is applied to the disk such that θ(t)=5t28t\theta(t) = 5t^2 - 8t, where θ(t)\theta(t) is the angular position of the rotating disk as a function of time tt. How much power is delivered by the applied torque, when t=2st = 2 \, \text{s}?

  • A

    60MR260MR^2

  • B

    72MR272MR^2

  • C

    108MR2108MR^2

  • D

    8MR28MR^2

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: θ(t)=5t28t\theta(t) = 5t^2 - 8t for a circular disk of mass MM and radius RR.

Find: Power delivered by the applied torque at t=2st = 2 \, \text{s}.

Use the relation

P=τωP = \tau \cdot \omega

First find the angular velocity:

ω(t)=dθ(t)dt=ddt(5t28t)=10t8\omega(t) = \frac{d\theta(t)}{dt} = \frac{d}{dt}(5t^2 - 8t) = 10t - 8

At t=2st = 2 \, \text{s},

ω(2)=10×28=12rad/s\omega(2) = 10 \times 2 - 8 = 12 \, \text{rad/s}

Now find the angular acceleration:

α(t)=dω(t)dt=ddt(10t8)=10\alpha(t) = \frac{d\omega(t)}{dt} = \frac{d}{dt}(10t - 8) = 10

For a circular disk about an axis perpendicular to its plane,

I=12MR2I = \frac{1}{2}MR^2

Torque is

τ=Iα=12MR2×10=5MR2\tau = I\alpha = \frac{1}{2}MR^2 \times 10 = 5MR^2

Therefore, power is

P=τω=5MR2×12=60MR2P = \tau \omega = 5MR^2 \times 12 = 60MR^2

Therefore, the power delivered is 60MR260MR^2 and the correct option is A.

Differentiate Once More and Substitute

Given: θ(t)=5t28t\theta(t) = 5t^2 - 8t.

Find: Power at t=2st = 2 \, \text{s}.

From the angular position,

ω=dθdt=10t8\omega = \frac{d\theta}{dt} = 10t - 8

so at t=2t = 2,

ω=12rad/s\omega = 12 \, \text{rad/s}

Also,

α=dωdt=10\alpha = \frac{d\omega}{dt} = 10

For the disk,

I=12MR2I = \frac{1}{2}MR^2

Hence,

τ=Iα=12MR2×10=5MR2\tau = I\alpha = \frac{1}{2}MR^2 \times 10 = 5MR^2

Now substitute directly into

P=τωP = \tau\omega

to get

P=5MR2×12=60MR2P = 5MR^2 \times 12 = 60MR^2

This works quickly because power in rotational motion depends directly on the instantaneous values of torque and angular speed. Hence the correct option is A.

Common mistakes

  • Using θ(t)\theta(t) directly in place of angular velocity. This is wrong because power depends on ω\omega, not on angular position. Differentiate θ(t)\theta(t) first to get ω(t)\omega(t).

  • Forgetting to compute angular acceleration from the derivative of ω(t)\omega(t). This is wrong because torque is obtained from τ=Iα\tau = I\alpha. After finding ω(t)\omega(t), differentiate once more to get α\alpha.

  • Using the wrong moment of inertia for a solid disk. This is wrong because for a disk about its central perpendicular axis, I=12MR2I = \frac{1}{2}MR^2, not MR2MR^2. Use the correct standard formula before calculating torque.

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