(d) Moment of inertia of cylinder about an axis through the centre and perpendicular to its axis is
$I_{c} = M\left( \frac{R^{2}}{4} + \frac{L^{2}}{12} \right)$
Using theorem of parallel axes, moment of inertia of the cylinder about an axis through its edge would be
$I = I_{c} + M\left( \frac{L}{2} \right)^{2} = M\left( \frac{R^{2}}{4} + \frac{L^{2}}{12} + \frac{L^{2}}{4} \right)$
$= M\left( \frac{R^{2}}{4} + \frac{L^{2}}{3} \right)$
When $L = 6\ R,\ I_{h} = \frac{49}{4}MR^{2}$