A particle starts oscillating simple harmonically from its equilibrium position with time period 'T'. What…
- $1: 2$
- $2: 1$
- $1: 3$
- $3: 1$
Solution
Given $\mathrm{t}=\frac{\mathrm{T}}{12}$ $\begin{aligned} \therefore \quad x & =A \sin \omega t=A \sin \frac{2 \pi}{T} \cdot t \\ \therefore \quad x & =A \sin \frac{2 \pi}{T} \times \frac{T}{12} \\ & =A \sin \left(\frac{\pi}{6}\right) \\ & =\frac{A}{2}...(iii) \end{aligned}$ Substituting equation (iii) in equation (i), $\begin{aligned} \text { P.E. } & =\frac{1}{2} \mathrm{~m} \omega^2\left(\frac{\mathrm{~A}^2}{4}\right) \\ & =\frac{\mathrm{m} \omega^2 \mathrm{~A}^2}{8} \end{aligned}$
Substituting equation (iii) in equation (ii), $\begin{aligned} \text { K.E. } & =\frac{1}{2} \mathrm{~m} \omega^2\left(\mathrm{~A}^2-\frac{\mathrm{A}^2}{4}\right) \\ & =\frac{1}{2} \mathrm{~m} \omega^2\left(\frac{3 \mathrm{~A}^2}{4}\right) \\ \therefore \quad \frac{\text { P.E. }}{\text { K.E. }} & =\frac{\frac{1}{2} m \omega^2 A^2 \times \frac{1}{4}}{\frac{1}{2} m \omega^2 A^2 \times \frac{3}{4}}=\frac{1}{3} \end{aligned}$ .
Asked in: MHT CET 2024 (10 May Shift 2)