To solve the problem, we need to find the time period of a particle executing Simple Harmonic Motion (SHM). The particle has an acceleration of \(12 \, \text{cm/s}^2\) at a distance of \(3 \, \text{cm}\) from the mean position.
The acceleration in SHM is given by the formula:
\(a = -\omega^2 x\)
where:
Given, \(a = 12 \, \text{cm/s}^2\) and \(x = 3 \, \text{cm}\).
Substituting these values into the formula:
\(12 = -\omega^2 \times 3\)
Simplifying, we get:
\(12 = -3 \omega^2\)
\(\omega^2 = -\frac{12}{3} = -4\)
\(\omega^2 = 4\)
\(\omega = 2 \text{ (as negative value indicates direction)}\)
The time period \((T)\) of SHM is related to angular frequency by the formula:
\(T = \frac{2\pi}{\omega}\)
Substitute \(\omega = 2\) into the equation:
\(T = \frac{2\pi}{2}\)
\(T = \pi \approx 3.14 \, \text{s}\)
Therefore, the time period is \(3.14 \, \text{s}\), which matches with option \(3.14 \, \text{s}\).
Conclusion: The time period of the particle in SHM is \(3.14 \, \text{s}\).