To solve the problem, we need to find the potential energy of the particle. Given that the particle is oscillating and has a mass \( m = 1 \) kg with a period \( T = \frac{\pi}{2} \), we assume simple harmonic motion. The potential energy (\( U \)) is provided by:
\( U = \frac{1}{2} k x^2 \)
where \( k \) is the spring constant, and \( x = 0.2 \) m is the displacement.
The period \( T \) of oscillation for a mass-spring system is:
\( T = 2\pi \sqrt{\frac{m}{k}} \)
Rearranging to find \( k \):
\( k = \frac{4\pi^2 m}{T^2} \)
Substituting the given values:
\( k = \frac{4\pi^2 \times 1}{\left(\frac{\pi}{2}\right)^2} \)
\( k = \frac{4\pi^2}{\frac{\pi^2}{4}} \)
\( k = 16 \)
Substituting back to find potential energy:
\( U = \frac{1}{2} \times 16 \times (0.2)^2 \)
\( U = 8 \times 0.04 \)
\( U = 0.32 \) J
Thus, the potential energy of the particle is \( 0.32 \) J.
Match the following