(d) In the given condition friction provides the required centripetal force and that is constant. $i.e.$ $m\omega^{2}r =$ constant
$\Rightarrow r \propto \frac{1}{\omega^{2}}\therefore r_{2} = r_{1}\left( \frac{\omega_{1}}{\omega_{2}} \right)^{2} = 9\left( \frac{1}{3} \right)^{2} = 1\ cm$