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Question: A wheel has a speed of 1200 revolutions per minute and is made to slow down at a rate of \(4{\text{r...

A wheel has a speed of 1200 revolutions per minute and is made to slow down at a rate of 4rads24{\text{rad}}{{\text{s}}^{ - 2}}. Find the number of revolutions it makes before coming to rest.
A) 143
B) 272
C) 314
D) 722

Explanation

Solution

The given speed of the wheel is actually the frequency of the rotation and the given rate at which the wheel slows down is its angular retardation. As the wheel comes to rest, we can take the final angular velocity of the wheel to be zero. The number of rotations made by the wheel can be calculated once the angular displacement of the wheel is known.

Formulas used:
The final angular velocity of a rotating body is given by, ωf2=ωi2+2αθ{\omega _f}^2 = {\omega _i}^2 + 2\alpha \theta , where ωi{\omega _i} is the initial angular velocity of the body, α\alpha is its angular acceleration and θ\theta is its angular displacement.
The number of rotation of a body is given by, n=θT2πn = \dfrac{{{\theta _T}}}{{2\pi }}, where θT{\theta _T} is the total angular displacement of the body.

Complete step by step answer:
Step 1: List the parameters given in the question.
The problem at hand involves a rotating wheel which slows down at a given rate and eventually comes to rest. We have to determine the number of rotations made by the wheel before it comes to a halt.
The frequency of the wheel is given to be f=1200rpmf = 1200{\text{rpm}}.
The angular retardation of the wheel is given to be α=4rads2\alpha = - 4{\text{rad}}{{\text{s}}^{ - 2}}.
Let ωi{\omega _i} be the initial angular velocity ωf=0{\omega _f} = 0 be the final angular velocity of the wheel.
Then we have ωi=2πf=2400πradmin1{\omega _i} = 2\pi f = 2400\pi {\text{radmi}}{{\text{n}}^{ - 1}}.
Let θT{\theta _T} be the total angular displacement of the wheel.
Step 2: Express the relation for the final angular velocity to obtain the angular displacement of the wheel.
The final angular velocity of the rotating wheel can be expressed as ωf2=ωi2+2αθ{\omega _f}^2 = {\omega _i}^2 + 2\alpha \theta .
θT=ωf2ωi22α\Rightarrow {\theta _T} = \dfrac{{{\omega _f}^2 - {\omega _i}^2}}{{2\alpha }} --------- (1)
Substituting for ωi=40πrads1{\omega _i} = 40\pi {\text{rad}}{{\text{s}}^{ - 1}}, ωf=0{\omega _f} = 0 and α=4rads2\alpha = - 4{\text{rad}}{{\text{s}}^{ - 2}} in equation (1) we get,
θT=0(40π)22×(4)=200π2m\Rightarrow {\theta _T} = \dfrac{{0 - {{\left( {40\pi } \right)}^2}}}{{2 \times \left( { - 4} \right)}} = 200{\pi ^2}{\text{m}}
Thus the angular displacement of the wheel is θT=200π2m{\theta _T} = 200{\pi ^2}{\text{m}}.
Step 3: Using the obtained angular displacement of the wheel, obtain the number of rotations performed by the wheel before stopping.
Let nn be the number of rotations performed by the wheel before coming to rest.
One rotation (n=1)\left( {n = 1} \right) corresponds to an angle θ=2π\theta = 2\pi .
So for the obtained angular displacement of the wheel, the number of rotations performed will be
n=θT2πn = \dfrac{{{\theta _T}}}{{2\pi }} ------- (2)
Substituting for θT=200π2m{\theta _T} = 200{\pi ^2}{\text{m}} and π=314\pi = 3 \cdot 14 in equation (2) we get,
n=200(314)22×314=314\Rightarrow n = \dfrac{{200{{\left( {3 \cdot 14} \right)}^2}}}{{2 \times 3 \cdot 14}} = 314
Thus the number of rotations is n=314n = 314.

Hence the correct option is C.

Note:
While substituting values of different physical quantities in an equation, all the quantities should be expressed in their respective S.I units. Here the initial velocity is converted into its S.I unit of radian per second as ωi=2400π60=40πrads1{\omega _i} = \dfrac{{2400\pi }}{{60}} = 40\pi {\text{rad}}{{\text{s}}^{ - 1}} before substituting in equation (1). Angular retardation is the negative of angular acceleration and so we substitute α=4rads2\alpha = - 4{\text{rad}}{{\text{s}}^{ - 2}} in equation (1).