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Question: A wheel has a constant angular acceleration of \(3.0rad/{s^2} \), During a certain \(4.0s \)interval...

A wheel has a constant angular acceleration of 3.0rad/s23.0rad/{s^2} , During a certain 4.0s4.0s interval, it turns through an angle of 120rad120rad . Assuming that at t=0t = 0 , angular speed ω0=3rad/s{\omega _0} = 3rad/s how long is motion at the start of this 4.04.0 second interval?
(A) 7s7s
(B) 9s9s
(C) 4s4s
(D) 10s10s

Explanation

Solution

Hint The angle of rotation of the wheel can be determined using the equations of circular motion. It is known that the difference between the initial and final angles is 120rad120rad , this can be put into the second equation of circular motion and solved for the time.
Formula used:
θ=ω0t+12αt2\theta = {\omega _0}t + \dfrac{1}{2}\alpha {t^2}
Where θ\theta is the angle covered by the rotating object.
ω0{\omega _0} is the initial angular velocity.
α\alpha is the angular acceleration.
tt is the time taken.

Complete Step by step answer
It is given in the question that,
The angular acceleration of the wheel is constant and is equal to α=3.0rad/s2\alpha = 3.0rad/{s^2}
The initial angular speed, ω0=3rad/s{\omega _0} = 3rad/s
Angle turned by the wheel in the given time interval, θ=120rad\theta = 120rad
Time interval given in the question is 4sec4\sec .
Let the start of the 4sec4\sec motion be at time tt .
Then the end of this motion happens at the time t+4t + 4
Let the initial angle of the wheel be θ1{\theta _1} and the final angle of the wheel be θ2{\theta _2} .
The total angle turned by the wheel can be written as-
120=θ2θ1120 = {\theta _2} - {\theta _1}
From the equation of circular motion, we know that-
θ=ω0t+12αt2\theta = {\omega _0}t + \dfrac{1}{2}\alpha {t^2}
For θ1{\theta _1} ,
θ1=3t+12×3t2{\theta _1} = 3t + \dfrac{1}{2} \times 3{t^2}
For θ2{\theta _2} ,
θ2=3(t+4)+12×3(t+4)2{\theta _2} = 3\left( {t + 4} \right) + \dfrac{1}{2} \times 3{\left( {t + 4} \right)^2}
Combining both of these equations by subtracting θ1{\theta _1} from θ2{\theta _2} ,
θ2θ1=(3(t+4)3t)+(32((t+4)2t2)){\theta _2} - {\theta _1} = \left( {3(t + 4) - 3t} \right) + \left( {\dfrac{3}{2}\left( {{{(t + 4)}^2} - {t^2}} \right)} \right)
θ2θ1=12+(32((t2+8t+16)t2)){\theta _2} - {\theta _1} = 12 + \left( {\dfrac{3}{2}\left( {({t^2} + 8t + 16) - {t^2}} \right)} \right)
θ2θ1=12+(32(8t+16)){\theta _2} - {\theta _1} = 12 + \left( {\dfrac{3}{2}\left( {8t + 16} \right)} \right)
120=12+32(8t+16)120 = 12 + \dfrac{3}{2}\left( {8t + 16} \right)
(108×23)16=8t\left( {108 \times \dfrac{2}{3}} \right) - 16 = 8t
t=72168=568=7t = \dfrac{{72 - 16}}{8} = \dfrac{{56}}{8} = 7

The motion of the wheel had started 77 seconds before the 4s4s time interval.

Note The equations of circular motion are similar to the equations of linear motion. Only the linear components are replaced with their angular counterparts. Like the distance in linear motion is replaced with the angle covered, linear velocity is replaced with angular velocity and the linear acceleration is replaced with angular acceleration.