JEE Challenger
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Rolling Motion of Cylinders with Different Mass Distributions

Two solid cylinders PP and QQ having equal mass and equal radius start rolling down a fixed inclined plane simultaneously from the same height. Cylinder PP has most of its mass concentrated near its outer surface, whereas cylinder QQ has most of its mass concentrated near its central axis. Which of the following statements is/are correct?

Options

A

Both cylinders PP and QQ reach the bottom of the incline at the same time.

B

Cylinder PP has a greater linear acceleration than cylinder QQ.

C

Both cylinders reach the bottom with equal translational kinetic energy.

D

Cylinder QQ reaches the bottom with a greater angular speed.

Correct

Step-by-Step Solution

To determine the correct statement(s), let us analyze the rotational motion of the two solid cylinders PP and QQ rolling down an inclined plane without slipping.

1. Comparison of Moments of Inertia

Let both cylinders have mass MM and radius RR.

  • Cylinder PP has most of its mass concentrated near its outer surface, meaning its mass is distributed at larger distances from the axis of rotation. Thus, its moment of inertia about the central axis, IPI_P, is larger.
  • Cylinder QQ has most of its mass concentrated near its central axis, meaning its mass is distributed closer to the axis of rotation. Thus, its moment of inertia, IQI_Q, is smaller.

Therefore, we have: IP>IQI_P > I_Q


2. Linear Acceleration

Consider a cylinder of mass MM, radius RR, and moment of inertia II rolling down a fixed inclined plane of angle θ\theta.

Using Newton's second law for translational and rotational motion: Mgsin⁡θ−f=MaM g \sin\theta - f = M a τ=fR=Iα\tau = f R = I \alpha

Since the cylinder rolls without slipping, the condition for pure rolling is a=αRa = \alpha R. Substituting α=aR\alpha = \frac{a}{R} into the torque equation gives: f=IaR2f = \frac{I a}{R^2}

Substituting the friction force ff back into the translational equation: Mgsin⁡θ−IaR2=MaM g \sin\theta - \frac{I a}{R^2} = M a a=gsin⁡θ1+IMR2a = \frac{g \sin\theta}{1 + \frac{I}{M R^2}}

Since IP>IQI_P > I_Q, the denominators satisfy: (1+IPMR2)>(1+IQMR2)\left(1 + \frac{I_P}{M R^2}\right) > \left(1 + \frac{I_Q}{M R^2}\right)

Hence, the linear accelerations are related by: aP<aQa_P < a_Q

  • Analysis of Option A: The time tt taken to travel a length SS along the incline starting from rest is t=2Sat = \sqrt{\frac{2S}{a}}. Since aQ>aPa_Q > a_P, cylinder QQ reaches the bottom in less time than cylinder PP (tQ<tPt_Q < t_P). Thus, Option A is incorrect.
  • Analysis of Option B: Cylinder QQ has a greater linear acceleration than cylinder PP (aQ>aPa_Q > a_P). Thus, Option B is incorrect.

3. Linear Velocity and Translational Kinetic Energy

The linear velocity vv at the bottom of an incline of height hh (where S=hsin⁡θS = \frac{h}{\sin\theta}) is given by: v2=2aS=2gh1+IMR2v^2 = 2 a S = \frac{2 g h}{1 + \frac{I}{M R^2}}

Since IP>IQI_P > I_Q, we find that: vQ>vPv_Q > v_P

The translational kinetic energy at the bottom is given by: Ktrans=12Mv2K_{\text{trans}} = \frac{1}{2} M v^2

Since vQ>vPv_Q > v_P and both cylinders have equal mass MM: Ktrans,Q>Ktrans,PK_{\text{trans}, Q} > K_{\text{trans}, P}

  • Analysis of Option C: Cylinder QQ reaches the bottom with greater translational kinetic energy than cylinder PP. Thus, Option C is incorrect.

4. Angular Speed

For pure rolling, the relationship between linear speed vv and angular speed ω\omega is: ω=vR\omega = \frac{v}{R}

Since vQ>vPv_Q > v_P and both cylinders have equal radius RR: ωQ=vQR>vPR=ωP\omega_Q = \frac{v_Q}{R} > \frac{v_P}{R} = \omega_P

  • Analysis of Option D: Cylinder QQ reaches the bottom with a greater angular speed (ωQ>ωP\omega_Q > \omega_P). Thus, Option D is correct.

Conclusion

The only correct option is D.