A particle moving in a circular path has an angular momentum of $L$. If the frequency of rotation is halved,…
- $\frac{\mathrm{L}}{2}$
- $\mathrm{L}$
- $\frac{L}{3}$
- $\frac{\mathrm{L}}{4}$
Solution
$\mathrm{L}=\mathrm{mr}^{2} \omega=2 \pi \mathrm{mr}^{2} \mathrm{f} \quad[\because \mathrm{W}=2 \pi \mathrm{f}]$
If frequency is halved then, $\mathrm{L}^{\prime}=\mathrm{mr}^{2} \frac{\omega}{2}=\pi \mathrm{mr}^{2} \mathrm{f} \therefore \mathrm{L}^{\prime}=\frac{\mathrm{L}}{2}$ .
Asked in: JEE Mains - Rotational Motion - Test 4