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A particle executes SHM with a time period T. If its maximum acceleration is doubled keeping the amplitude constant, its new time period is

  • A.\(T\)
  • B.\(2T\)
  • C.\(\frac{T}{2}\)
  • D.\(\frac{T}{\sqrt{2}}\)
  • E.\(\sqrt{2}T\)

Answer: D

The new time period is \(\frac{T}{\sqrt{2}}\).

In SHM the maximum acceleration is \(a_{max} = \omega^{2}A\). With A fixed, doubling \(a_{max}\) doubles \(\omega^{2}\).

\[ \begin{aligned} \omega'^{2} &= 2\omega^{2} \Rightarrow \omega' = \sqrt{2}\,\omega \\ T' &= \frac{2\pi}{\omega'} = \frac{T}{\sqrt{2}} \end{aligned} \]

\(\frac{T}{2}\) would need \(\omega\) to double, which means \(a_{max}\) four times larger. \(\sqrt{2}T\) and 2T go the wrong way: a larger restoring acceleration makes the motion faster, not slower.

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