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Question: A wheel having moment of inertia\(2\,kg\,{{m}^{2}}\) about its vertical axis, rotates at the rate of...

A wheel having moment of inertia2kgm22\,kg\,{{m}^{2}} about its vertical axis, rotates at the rate of 60rpm60\,rpm about its axis. The torque which can stop the wheel’s rotation in one minute would be-
(A). 2π13Nm\dfrac{2\pi }{13}N\,m
(B). π14Nm\dfrac{\pi }{14}N\,m
(C). π15Nm\dfrac{\pi }{15}N\,m
(D). π20Nm\dfrac{\pi }{20}N\,m

Explanation

Solution

The wheel is undergoing pure angular motion; it does not show translational motion. According to the second law of motion, a force is required to change the state of rest or motion of a body. Here, torque is analogous to force, this means an external torque is required to bring the wheel at rest.

Formulas used:
ω=ω0+αt\omega ={{\omega }_{0}}+\alpha t
τ=Iα\tau =I\alpha

Complete step-by-step solution:
A wheel is rotating about a vertical axis passing through its centre. Its angular velocity is-
60rpm=60×2π1×60rads1 60rpm=2πrads1 \begin{aligned} & 60rpm=\dfrac{60\times 2\pi }{1\times 60}rad\,{{s}^{-1}} \\\ & \therefore 60rpm=2\pi \,rad\,{{s}^{-1}} \\\ \end{aligned}
Given, its moment of inertia is,I=2kgm2I=2\,kg\,{{m}^{2}}
Since no external force is acting on the system of the wheel, its angular acceleration is constant.
Using equations for angular motion along an axis,
ω=ω0+αt\omega ={{\omega }_{0}}+\alpha t
Here,
ω\omega is the final angular velocity
ω0{{\omega }_{0}} is the initial angular velocity
α\alpha is the angular acceleration
tt is time taken
The wheel is to be stopped, therefore ω=0\omega =0
We substitute the given values in the above equation to get,
ω=ω0+αt 0=2π+α×60 α=2π60 α=π30rads2 \begin{aligned} & \omega ={{\omega }_{0}}+\alpha t \\\ & \Rightarrow 0=2\pi +\alpha \times 60 \\\ & \Rightarrow \alpha =-\dfrac{2\pi }{60} \\\ & \therefore \alpha =-\dfrac{\pi }{30}rad\,{{s}^{-2}} \\\ \end{aligned} [1 minute = 60secs]
The wheel will have to undergo deceleration of π30rads2\dfrac{\pi }{30}rad\,{{s}^{-2}} to come to rest in 1 minute.
The torque required to bring the wheel at rest is given by-
τ=Iα\tau =I\alpha
Here,
τ\tau is the torque
II is the moment of inertia
Therefore, we substitute values in the above equation to get,
τ=Iα τ=2×π30 τ=π15Nm \begin{aligned} & \tau =I\alpha \\\ & \Rightarrow \tau =2\times \dfrac{\pi }{30} \\\ & \therefore \tau =\dfrac{\pi }{15}\,N\,m \\\ \end{aligned}
The torque required to bring the wheel at rest isπ15Nm\dfrac{\pi }{15}\,N\,m.

Hence, the correct option is (C).

Note:
The torque must be applied in the direction opposite to the motion of the wheel. The moment of inertia, also called the angular mass is a quantity which is used to determine the torque needed for an angular acceleration. The linear velocity of the wheel is tangential to its motion. The equations of angular motion of a body are analogous to the equations of motion in a straight line.