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The equation of rotational motion for constant angular acceleration is given by
ωf2 = ωi2 + 2αθ
⇒ θ = \(\frac{\omega_f^2 - \omega_i^2}{2 \alpha}\)
Where
- ωf = final angular velocity
- ωi = initial angular velocity
- α = angular acceleration
- θ = angular displacement of the body during the time in which its angular velocity
Changes from ωi to ωf
Given,
Initial angular velocity of the fan, ωi = 5 rad/s
final angular velocity of the fan, ωf = 15 rad/s
Angular acceleration, α = 1 rad/sec2
Using the equation of rotational motion, angular displacement of the fan, is given by
θ = \(\frac{15^2-5^2}{2 \times 1}\) = \(\frac{225-25}{2}\) = 100 rad
Hence, the body rotates angular displacement of 100 rad during the time in which its angular velocity increases from 5 rad/s to 15 rad/s.
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