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Question: A body rotates about a fixed axis with an angular acceleration of \( 3rad/{s^2} \) . The angle rotat...

A body rotates about a fixed axis with an angular acceleration of 3rad/s23rad/{s^2} . The angle rotated by it during the time when its angular velocity increases from 10 rad/s to 20 rad/s (in radians) is
(A) 50
(B) 150
(C) 200
(D) 100

Explanation

Solution

The rotational equivalent of the equation of motion could be utilized to solve the problem. This can simply be done by replacing all the linear quantities in the equation with their rotational counterpart.

Formula used: In this solution we will be using the following formulae;
ω2=ω02+2αθ{\omega ^2} = \omega _0^2 + 2\alpha \theta where ω\omega is the final angular speed of a rotating body, ω0{\omega _0} is the initial angular speed of the body, α\alpha is the angular acceleration of the body, and θ\theta is the angular displacement.
v2=u2+2as{v^2} = {u^2} + 2as where vv is the final linear velocity, uu is the initial, aa is the linear acceleration and ss is the distance travelled.

Complete step by step answer:
To solve the above problem, one can use the rotational equivalent of the third equation of motion which can be written as
ω2=ω02+2αθ{\omega ^2} = \omega _0^2 + 2\alpha \theta where ω\omega is the final angular speed of a rotating body, ω0{\omega _0} is the initial angular speed of the body, α\alpha is the angular acceleration of the body, and θ\theta is the angular displacement.
Hence, from the question, we can insert all known values, as in
202=102+2(3)θ{20^2} = {10^2} + 2\left( 3 \right)\theta
Hence, by calculating, and making θ\theta the subject of the formula, we have that
400=100+2(3)θ400 = 100 + 2\left( 3 \right)\theta
θ=4001002(3)=3006=50rad\theta = \dfrac{{400 - 100}}{{2\left( 3 \right)}} = \dfrac{{300}}{6} = 50rad
Hence, the angular displacement is 50 rad
Thus, the correct option is A.

Note:
For clarity, we can get the rotational equation of motion by simply substituting the rotational counterparts of all the linear quantities in place of the linear quantities. For example, for the third equation of motion, we have
v2=u2+2as{v^2} = {u^2} + 2as where vv is the final linear velocity, uu is the initial, aa is the linear acceleration and ss is the distance travelled.
Hence, we replace vv with ω\omega , uu with ω0{\omega _0} , aa with α\alpha , and ss with θ\theta . Hence, we have
ω2=ω02+2αθ{\omega ^2} = \omega _0^2 + 2\alpha \theta .