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Question: When a ceiling fan is switched off, its angular velocity falls to half while it makes 36 rotations H...

When a ceiling fan is switched off, its angular velocity falls to half while it makes 36 rotations How many more rotations will it make before coming to rest.
A) 2424
B) 3636
C) 1818
D) 1212

Explanation

Solution

We solve this question in two parts first we consider when the fan is switched off then its velocity becomes half of its initial velocity before this it makes 3636 round for this part we apply the equation of rotational motion. And in the second time we consider when its angular velocity is half and it becomes after some time zero means it comes to rest considering it makes nn round before stop. We want to calculate this no of round which it completes before stopping.

Complete step by step solution:
We assume that the initial angular velocity of fan just after switching off the fan is ω\omega
When it complete 3636 round its angular velocity decrease to ω2\dfrac{\omega }{2} lets assume angular acceleration is α\alpha
Third equation of rotational motion for retarded motion
ω2=ω202αθ\Rightarrow {\omega ^2} = {\omega ^2}_0 - 2\alpha \theta
Where ω\omega final angular velocity and ω0{\omega _0} is initial angular velocity ,α\alpha denotes angular acceleration and θ\theta is angular displacement
For this case initial angular velocity is =ω= \omega
Final angular velocity is ω2\dfrac{\omega }{2}
Angular displacement in 36 round is 36×2π36 \times 2\pi
Put these value in above equation
(ω2)2=(ω)22(α)(36×2π)\Rightarrow {\left( {\dfrac{\omega }{2}} \right)^2} = {\left( \omega \right)^2} - 2\left( \alpha \right)\left( {36 \times 2\pi } \right)
2(α)(36×2π)=(ω)2(ω2)2\Rightarrow 2\left( \alpha \right)\left( {36 \times 2\pi } \right) = {\left( \omega \right)^2} - {\left( {\dfrac{\omega }{2}} \right)^2}
Solving this
2(α)(36×2π)=ω2ω24\Rightarrow 2\left( \alpha \right)\left( {36 \times 2\pi } \right) = {\omega ^2} - \dfrac{{{\omega ^2}}}{4}
2(α)(36×2π)=(4ω2ω2)4\Rightarrow 2\left( \alpha \right)\left( {36 \times 2\pi } \right) = \dfrac{{\left( {4{\omega ^2} - {\omega ^2}} \right)}}{4} ........... (1)

Step 2
Now we take second half part in which fan get rest from ω2\dfrac{\omega }{2} angular velocity
Let us assume it rotate nn round before stop means angular displacement θ=2π(n)\theta = 2\pi \left( n \right)
Initial angular velocity ω2\dfrac{\omega }{2}
Final angular velocity 00
Apply equation of motion
(0)2=(ω2)22(α)(n×2π)\Rightarrow {\left( 0 \right)^2} = {\left( {\dfrac{\omega }{2}} \right)^2} - 2\left( \alpha \right)\left( {n \times 2\pi } \right)
2(α)(n×2π)=ω24\Rightarrow 2\left( \alpha \right)\left( {n \times 2\pi } \right) = \dfrac{{{\omega ^2}}}{4} .................. (2)
Divide equation (1) by (2) then
2(α)(36×2π)2(α)(n×2π)=(4ω2ω2)(ω2)\Rightarrow \dfrac{{2\left( \alpha \right)\left( {36 \times 2\pi } \right)}}{{2\left( \alpha \right)\left( {n \times 2\pi } \right)}} = \dfrac{{\left( {4{\omega ^2} - {\omega ^2}} \right)}}{{\left( {{\omega ^2}} \right)}}
Further solving
36n=ω2(41)ω2\Rightarrow \dfrac{{36}}{n} = \dfrac{{{\omega ^2}\left( {4 - 1} \right)}}{{{\omega ^2}}}
Solving this equation
3n=36\Rightarrow 3n = 36
n=363 n=12  \therefore n = \dfrac{{36}}{3} \\\ \therefore n = 12 \\\
Hence option (D) is correct.

Note: Angular displacement is the angle in radian swap by radius arm on centre. We use here angular displacement relation with round of fan how can be relate round of fan with angular displacement it is given below:
We know angular displacement in one round is 2π2\pi radian.
So angular displacement θ\theta in nn round is n×2πn \times 2\pi radian.