(a) $U = k|x|^{3} \Rightarrow F = - \frac{dU}{dx} = - 3k|x|^{2}$ …(i)
Also, for SHM $x = a\sin{\omega t}$ and$\ \frac{d^{2}x}{dt^{2}} + \omega^{2}x = 0$
$\Rightarrow$ acceleration $a = \frac{d^{2}x}{dt^{2}} = - \omega^{2}x \Rightarrow F = ma$
$= m\frac{d^{2}x}{dt^{2}} = - m\omega^{2}x\ \ \ \ \ \ $ …(ii)
From equation (i) & (ii) we get $\omega = \sqrt{\frac{3kx}{m}}$
$\Rightarrow T = \frac{2\pi}{\omega} = 2\pi\sqrt{\frac{m}{3kx}} = 2\pi\sqrt{\frac{m}{3k(a\sin{\omega t})}} \Rightarrow T \propto \frac{1}{\sqrt{a}}$