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In a simple harmonic motion, let \(\mathrm{f}\) be the acceleration and \(\mathrm{T}\) be the time period. If \(x\) denotes the displacement, then |fT| vs. X graph will look like,
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\(\begin{gathered}\text {Hint: } F \cdot T=\omega^2 x \cdot \frac{2 \pi}{\omega}=2 \pi \omega x \\ \because \text { F.T }=2 \pi \omega x\end{gathered}\)


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