Question:

A grindstone has a moment of inertia of $6 \,kg\, m^2$. A constant torque is applied and the grindstone is found to have a speed of $150\, rpm, 10$ seconds after starting from rest. The torque is

Updated On: Feb 11, 2024
  • $3 \pi \,N \,m$
  • $3 \,N\,m$
  • $ \frac{\pi}{3} \,N \,m$
  • $4 \pi \,N \,m$
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The Correct Option is A

Solution and Explanation

Here, $I = 6 \,kg\, m^{2}, t = 10\, s, \omega_{0} = 0$ $ \upsilon = 150 \,rpm = \frac{150}{60} \,rps = \frac{5}{2}\, rps $ $ \omega = 2\pi\upsilon = 2\pi \times\frac{5}{2} = 5\pi\, rad\, s^{-1} $ $ \alpha = \frac{\omega-\omega_{0}}{t} = \frac{5\pi -0}{10} = \frac{\pi}{2}rad\, s^{-2}$ $ \therefore$ Torque, $\tau = I \alpha = 6 \times\frac{\pi}{2} = 3\pi N m$
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Concepts Used:

System of Particles and Rotational Motion

  1. The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
  2. The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.