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Question: A circular disc is rotating about its own axis at uniform angular velocity\[\omega \]. The disc is s...

A circular disc is rotating about its own axis at uniform angular velocityω\omega . The disc is subjected to uniform angular retardation by which its angular velocity is decreased to ω2\dfrac{\omega }{2}during 120    120\;\;rotations. The number of rotations further made by it before coming to rest is:
A. 120    120\;\;
B. 60    60\;\;
C. 4040
D. 2020

Explanation

Solution

Given that the disc is rotating about its axis. Uniform angular retardation is acting on the rotating disc. Retardation means the final velocity of the body is reduced when compared to the initial velocity. Retardation can also be termed as deceleration or negative acceleration. Therefore it is obvious that this retardation will reduce the rotations of the disc. Let us see how many rotations that disc will make after the retardation.

Complete step by step solution:
Given that the initial angular velocity . After the angular retardation, the disc’s angular velocity is reduced by ω2\dfrac{\omega }{2}. Also initially the number of rotations of the disc is 120    120\;\;. We need to find the number of rotations of the disc after the retardation.
We know the third equation of motion,
v2=u2+2as.{v^2} = {u^2} + 2as.
Here vv is the final velocity, uu is the initial velocity, aa is the acceleration, ss is the displacement.
The above equation is for linear motion, for rotational motion the above equation becomes,
ω22=ω12+2αθ{\omega _2}^2 = {\omega _1}^2 + 2\alpha \theta
Here ω2{\omega _2} is the said to be final angular velocity, ω1{\omega _1} is said to be the initial angular velocity, α\alpha is the angular acceleration, θ\theta is the angular displacement.
We can rearrange the above equation to find the angular acceleration as,
α=ω12ω222θ1\alpha = \dfrac{{{\omega _1}^2 - {\omega _2}^2}}{{2{\theta _1}}}
Here it is said that the disc is subjected to uniform retardation.
Therefore α\alpha here is the angular retardation which is constant.
Similarly, we can write for the above equation after the angular retardation.
α=ω22ω322θ2\alpha = \dfrac{{{\omega _2}^2 - {\omega _3}^2}}{{2{\theta _2}}}
Equating both the equations.
ω12ω222θ1=ω22ω322θ2\dfrac{{{\omega _1}^2 - {\omega _2}^2}}{{2{\theta _1}}} = \dfrac{{{\omega _2}^2 - {\omega _3}^2}}{{2{\theta _2}}}
Here, ω3{\omega _3} is the case in which the disc comes to rest. Therefore ω3=0{\omega _3} = 0
Also θ1=1200{\theta _1} = {120^0}
ω2=ω12{\omega _2} = \dfrac{{{\omega _1}}}{2}
Therefore we can say that ω1=ω{\omega _1} = \omega and ω2=ω2{\omega _2} = \dfrac{\omega }{2}. Substituting all the values we get,
ω2(ω2)22θ1=(ω2)22θ2\dfrac{{{\omega ^2} - {{(\dfrac{\omega }{2})}^2}}}{{2{\theta _1}}} = \dfrac{{{{(\dfrac{\omega }{2})}^2}}}{{2{\theta _2}}}
Solving the above equation we get,
θ2=θ13{\theta _2} = \dfrac{{{\theta _1}}}{3}
θ2=1203{\theta _2} = \dfrac{{120}}{3}
θ2=40{\theta _2} = 40
Therefore the disc will make 4040 rotations further made by it before coming to rest.
Therefore the correct option is C.

Note:
One should know the difference between retardation and acceleration. Retardation means the reduction of the velocity of the body which means the final velocity is less than the initial velocity. Acceleration means an increase in velocity of the body which means the final velocity is greater than the initial velocity.