(a) By the theorem of perpendicular axes, the moment of inertia about the central axis $I_{C}$, will be equal to the sum of its moments of inertia about two mutually perpendicular diameters lying in its plane.
Thus, $I_{d} = I = \frac{1}{2}MR^{2}$
$\therefore$ $I_{C} = I + I$
$= \frac{1}{2}MR^{2} + \frac{1}{2}MR^{2}\ $
$= I + I = 2I$