(b) Here, $y = \sin^{2}{\omega t}$
$\frac{dy}{dt} = 2\omega\sin{\omega t\cos{\omega t = \omega\sin{2\omega t}}}$
[image:15_image74.emf]
$\frac{d^{2}y}{dt^{2}} = 2\omega^{2}\cos{2\omega t}$
For SHM, $\frac{d^{2}y}{dt^{2}} \propto - y$
Hence, function is not SHM, but periodic, From the $y - t$ graph, time period is
$t = \frac{\pi}{\omega}$