A particle of mass 40 g executes simple harmonic motion with an amplitude of 2.0 cm. If the time period of oscillation is \( \frac{\pi}{20} \) s, the total mechanical energy of the system is:
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In SHM, total mechanical energy remains constant and depends on amplitude squared.
The total energy in SHM is given by:
\[
E = \frac{1}{2} k A^2
\]
where \( k = m\omega^2 \) and \( \omega = \frac{2\pi}{T} \). Given \( T = \frac{\pi}{20} \):
\[
\omega = \frac{2\pi}{\frac{\pi}{20}} = 40
\]
\[
k = m\omega^2 = 0.04 \times 40^2 = 64 { N/m}
\]
Substituting \( A = 0.02 \) m:
\[
E = \frac{1}{2} \times 64 \times (0.02)^2 = 0.0128 { J} = 12.8 { mJ}
\]
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