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Question: A wheel starting from rest is uniformly accelerated at \(4rad/{{s}^{2}}\) for 10seconds. It is allow...

A wheel starting from rest is uniformly accelerated at 4rad/s24rad/{{s}^{2}} for 10seconds. It is allowed to rotate uniformly for the next 10 seconds and is finally brought to rest in the next 10seconds. Then the total angle rotated by the wheel is
A. 600rad
B. 800rad
C. 400rad
D. 200rad

Explanation

Solution

As a first step, you could read the question carefully and note down all the given values in the question. Then, you could divide the whole motion into three parts and do the calculations accordingly. So, you could find the angle rotation that took place in each part and then take their sum to get the net rotation.
Formula used:
Angular acceleration,
α=ΔωΔt\alpha =\dfrac{\Delta \omega }{\Delta t}
Angle rotated,
θ=ωf2ωi22α\theta =\dfrac{{{\omega }_{f}}^{2}-{{\omega }_{i}}^{2}}{2\alpha }

Complete step-by-step solution:
In the question we are actually given details about three sets of motion which are: uniformly accelerated motion, constant angular velocity and then uniform deceleration.
(A) Uniformly accelerated motion,
ωi=0{{\omega }_{i}}=0
t=10st=10s
α=4rad/s2\alpha =4rad/{{s}^{2}}
ωf=αt=40rad/s{{\omega }_{f}}=\alpha t=40rad/s
Now for finding the angle rotated by the wheel in the part of the motion,
ωf2ωi2=2αθ1{{\omega }_{f}}^{2}-{{\omega }_{i}}^{2}=2\alpha {{\theta }_{1}}
40202=2×4×θ1\Rightarrow {{40}^{2}}-{{0}^{2}}=2\times 4\times {{\theta }_{1}}
θ1=16008=200rad\therefore {{\theta }_{1}}=\dfrac{1600}{8}=200rad
So, we found the angular rotated in this part of the motion to be 200radian.
(B) Constant angular velocity,
ω=40rad/s\omega =40rad/s
ω=ΔθΔt=Δθ10=40rad/s\omega =\dfrac{\Delta \theta }{\Delta t}=\dfrac{\Delta \theta }{10}=40rad/s
Δθ2=400rad\therefore \Delta {{\theta }_{2}}=400rad
We found the angle rotated in this part of the motion to be 400radian.
(C) Uniformly decelerated motion,
ωi=40rad/s{{\omega }_{i}}=40rad/s
ωf=0{{\omega }_{f}}=0
t=10st=10s
Now we have angular acceleration as,
α=ΔωΔt=04010=4\alpha =\dfrac{\Delta \omega }{\Delta t}=\dfrac{0-40}{10}=-4
Now for finding the angle rotated here,
ωf2ωi2=2αΔθ{{\omega }_{f}}^{2}-{{\omega }_{i}}^{2}=2\alpha \Delta \theta
02402=2(4)Δθ3\Rightarrow {{0}^{2}}-{{40}^{2}}=2\left( -4 \right)\Delta {{\theta }_{3}}
θ3=16008=200rad\therefore {{\theta }_{3}}=\dfrac{1600}{8}=200rad
Angle rotated here is found to be 200radian.
So, the total rotation that is caused would be,
θtotal=θ1+θ2+θ3=200+400+200{{\theta }_{total}}={{\theta }_{1}}+{{\theta }_{2}}+{{\theta }_{3}}=200+400+200
θtotal=800radian\therefore {{\theta }_{total}}=800radian
Hence, the total angle rotated by the wheel is 800radian. Option B is correct.

Note: In case if you wonder how we divided the whole motion into three parts you could read the question again. The question clearly indicates that the wheel starts rotating from rest, and then undergoes uniform rotation and finally the wheel goes to rest each part happens in an interval of 10s.