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Question: A dumbbell consists of two identical particles of mass m connected by a rigid light rod of length 2 ...

A dumbbell consists of two identical particles of mass m connected by a rigid light rod of length 2 l. The dumbbell is set spinning with angular speed ω0\omega_0 on a surface with a small friction coefficient μk\mu_k. At what time (in sec) dumbbell stop. (ω0\omega_0 = 8 rad/sec, l = 1m, μk\mu_k = 0.4)

Answer

2.04

Explanation

Solution

The dumbbell consists of two identical particles of mass mm at a distance ll from the center, connected by a light rod of length 2l2l. The axis of rotation passes through the center of the rod.

  1. Moment of Inertia (I): The moment of inertia of the dumbbell about the axis of rotation is the sum of the moments of inertia of the two particles. For a point mass mm at a distance rr from the axis, I=mr2I = mr^2. Therefore, I=m(l)2+m(l)2=2ml2I = m(l)^2 + m(l)^2 = 2ml^2.

  2. Frictional Torque (τ\tau): The kinetic friction force on each particle is fk=μkNf_k = \mu_k N, where NN is the normal force. Since the particles are on a surface, N=mgN = mg. So, fk=μkmgf_k = \mu_k mg. This friction force acts tangentially, opposing the motion, at a distance ll from the axis of rotation. The torque due to friction on one particle is τ1=fk×l=(μkmg)×l\tau_1 = f_k \times l = (\mu_k mg) \times l. Since there are two such particles, the total frictional torque is τ=2×(μkmgl)=2μkmgl\tau = 2 \times (\mu_k mgl) = 2\mu_k mgl. This torque causes angular deceleration.

  3. Angular Deceleration (α\alpha): Using Newton's second law for rotation, τ=Iα\tau = I\alpha. The torque opposes the angular velocity, so we consider its magnitude. α=τI=2μkmgl2ml2=μkgl\alpha = \frac{\tau}{I} = \frac{2\mu_k mgl}{2ml^2} = \frac{\mu_k g}{l}.

  4. Time to Stop (t): We use the rotational kinematic equation ωf=ω0+αt\omega_f = \omega_0 + \alpha t, where ωf\omega_f is the final angular velocity, ω0\omega_0 is the initial angular velocity, and α\alpha is the angular acceleration. Since the dumbbell stops, ωf=0\omega_f = 0. The acceleration is negative as it opposes the motion. 0=ω0αt0 = \omega_0 - \alpha t t=ω0α=ω0μkgl=ω0lμkgt = \frac{\omega_0}{\alpha} = \frac{\omega_0}{\frac{\mu_k g}{l}} = \frac{\omega_0 l}{\mu_k g}.

  5. Given Values: ω0=8\omega_0 = 8 rad/sec l=1l = 1 m μk=0.4\mu_k = 0.4 We use the standard value for acceleration due to gravity, g=9.8g = 9.8 m/s².

  6. Calculation: t=8 rad/sec×1 m0.4×9.8 m/s2=83.92 sec2.04 sect = \frac{8 \text{ rad/sec} \times 1 \text{ m}}{0.4 \times 9.8 \text{ m/s}^2} = \frac{8}{3.92} \text{ sec} \approx 2.04 \text{ sec}.