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A particle of mass $m$ executes simple harmonic motion with amplitude ' $a$ ' and frequency ' $v$ '. The average kinetic energy during its motion from the position of equilibrium to the end is
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The correct answer is:
$\pi^2 \mathrm{ma}^2 v^2$
$\pi^2 \mathrm{ma}^2 v^2$
$\frac{1}{4} m a^2 \omega^2=\pi^2 f^2 m a^2$
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