For simple harmonic motion (SHM), the total mechanical energy is given by the sum of the kinetic and potential energies. When the object crosses the mean position, its kinetic energy is maximum and potential energy is zero. The kinetic energy at the mean position is:
\[
K.E = \frac{1}{2} m \omega^2 A^2
\]
where:
- \( m = 3 \, \text{kg} \) (mass),
- \( A = \frac{2}{\pi} \, \text{m} \) (amplitude),
- \( \omega = 2\pi f \) (angular frequency),
- \( f \) is the frequency.
Given that the kinetic energy at the mean position is 6 J, we can set up the equation:
\[
6 = \frac{1}{2} \times 3 \times (2\pi f)^2 \times \left( \frac{2}{\pi} \right)^2
\]
Simplifying:
\[
6 = \frac{1}{2} \times 3 \times 4 \pi^2 f^2 \times \frac{4}{\pi^2}
\]
\[
6 = 24 f^2
\]
\[
f^2 = \frac{1}{4} \quad \Rightarrow \quad f = \frac{1}{2} \, \text{Hz}
\]
The time period \( T \) is the reciprocal of the frequency:
\[
T = \frac{1}{f} = \frac{1}{\frac{1}{2}} = 2 \, \text{s}
\]
Thus, the time period of the oscillation is \( 2 \, \text{s} \), and the correct answer is option (2).