(d) For moving on circular path without slipping, centripetal force must equal frictional force
That is,
$\frac{mv^{2}}{r} = \mu\ m\ g$
$\Rightarrow mr\omega^{2} = \mu\ m\ g$ $\lbrack\therefore v = r\ \omega\rbrack$
$\Rightarrow r\ \omega^{2} = \ \mu\ g$
$\therefore\ \omega = \sqrt{\frac{\mu\ g}{r}} = \sqrt{\frac{0.5 \times 9.8}{10}} = 0.7\ rad/s$