(c) The relation between acceleration ($a$) and displacement ($x$) for a body in SHM is
$a = - \omega^{2}x$
Given, $a = - bx$
On comparing the two equations, we get
$\omega^{2} = b$
$\therefore$ $\omega = \sqrt{b}$
Since, $\omega = \frac{2\pi}{T}$
$\therefore$ $\frac{2\pi}{T} = \sqrt{b}$
$\Rightarrow \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ T = \frac{2\pi}{\sqrt{b}}$