A simple pendulum has a periodic time ' $\mathrm{T}_1$ ' when it is on the surface of earth of radius ' $R$…
- $\sqrt{2}$
- 1
- 2
- $\frac{1}{2}$
Solution
At a height ' $h=2 R$ ' from earth's surface, $\begin{aligned} & \mathrm{T}_2=2 \pi \sqrt{\frac{l}{\mathrm{~g}_{\mathrm{h}}}} \\ & \therefore \quad \frac{\mathrm{~T}_2}{\mathrm{~T}_1}=\sqrt{\frac{\mathrm{g}}{\mathrm{~g}_{\mathrm{h}}}}...(i) \\ & \text { Now, } \mathrm{g}_{\mathrm{h}}=\frac{\mathrm{GM}}{(\mathrm{R}+\mathrm{h})^2} \\ & \therefore \quad \mathrm{~g}_{\mathrm{h}}=\frac{\mathrm{GM}}{4 \mathrm{R}^2} \\ & \therefore \quad \mathrm{~g}_{\mathrm{h}}=\frac{\mathrm{g}}{4} \quad \ldots .(\because \mathrm{R}+\mathrm{h}=2 \mathrm{R}) \\ & \therefore \quad \ldots(\text { (ii) } \end{aligned}$ $\therefore \quad$ From equations (i) and (ii), $\frac{T_2}{T_1}=\sqrt{\frac{g}{g / 4}}=2$
Asked in: MHT CET 2024 (16 May Shift 1)