AIPMT PRELIMS2004Physics-Rotational Motion

AIPMT PRELIMS 2004 Physics Torque MCQ Question

Type: MCQ-numerical-Medium-Class 11

A wheel having moment of inertia 2 kg–m² about its vertical axis, rotates at the rate of 60 rpm about the axis. The torque which can stop the wheel's rotation in one minute would be :-

A

π/12 N–m

B

π/15 N–m

C

π/18 N–m

D

2π/15 N–m

Correct Answer

Option B

Detailed Explanation

To solve the problem of determining the torque required to stop a rotating wheel in one minute, we need to apply the concepts of rotational motion, specifically the relationship between torque, moment of inertia, angular velocity, and angular acceleration.

Given Data:

  • Moment of inertia, I=2kgm2I = 2 \, \text{kg} \cdot \text{m}^2
  • Initial angular velocity, ωi=60rpm\omega_i = 60 \, \text{rpm}
  • Time to stop, t=1minute=60secondst = 1 \, \text{minute} = 60 \, \text{seconds}

Step 1: Convert Angular Velocity to Radians per Second

The angular velocity in revolutions per minute (rpm) must be converted to radians per second (rad/s). We use the conversion factor:

1rpm=2πrad60s1 \, \text{rpm} = \frac{2\pi \, \text{rad}}{60 \, \text{s}}

Thus,

ωi=60rpm=60×2πrad60s=2πrad/s\omega_i = 60 \, \text{rpm} = 60 \times \frac{2\pi \, \text{rad}}{60 \, \text{s}} = 2\pi \, \text{rad/s}

Step 2: Determine Angular Deceleration

To stop the wheel, we need to decelerate it from ωi\omega_i to ωf=0rad/s\omega_f = 0 \, \text{rad/s} over a time period of t=60st = 60 \, \text{s}. The angular acceleration α\alpha can be calculated using the formula:

α=Δωt=ωfωit\alpha = \frac{\Delta \omega}{t} = \frac{\omega_f - \omega_i}{t}

Substituting the values:

α=02π60=2π60=π30rad/s2\alpha = \frac{0 - 2\pi}{60} = -\frac{2\pi}{60} = -\frac{\pi}{30} \, \text{rad/s}^2

Step 3: Calculate Required Torque

The torque τ\tau required to produce this angular acceleration can be calculated using Newton’s second law for rotation:

τ=Iα\tau = I \cdot \alpha

Substituting the known values:

τ=2kgm2(π30rad/s2)=2π30Nm\tau = 2 \, \text{kg} \cdot \text{m}^2 \cdot \left(-\frac{\pi}{30} \, \text{rad/s}^2\right) = -\frac{2\pi}{30} \, \text{N} \cdot \text{m}

Taking the magnitude, we find:

τ=2π30=π15Nm\tau = \frac{2\pi}{30} = \frac{\pi}{15} \, \text{N} \cdot \text{m}

Conclusion

Thus, the torque required to stop the wheel in one minute is:

π15Nm\boxed{\frac{\pi}{15} \, \text{N} \cdot \text{m}}

Explanation of Options

  • Option A: π12Nm\frac{\pi}{12} \, \text{N} \cdot \text{m}: Incorrect, as it does not match the calculated torque.
  • Option B: π15Nm\frac{\pi}{15} \, \text{N} \cdot \text{m}: Correct, matches our calculation.
  • Option C: π18Nm\frac{\pi}{18} \, \text{N} \cdot \text{m}: Incorrect, as it is less than the required torque.
  • Option D: 2π15Nm\frac{2\pi}{15} \, \text{N} \cdot \text{m}: Incorrect, as it is greater than the required torque.

In conclusion, the torque needed to stop the wheel within one minute is indeed π15Nm\frac{\pi}{15} \, \text{N} \cdot \text{m}, confirming that option B is the correct answer.

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