Consider a thin uniform disc of mass M and radius R in the xy plane. Let Ix, ly and Iz be the moments of inertia of the disc about the x, y and z axes respectively.
Now, Ix = Iy
since each represents the moment of inertia (MI) of the disc about its diameter and, by symmetry, the MI of the disc about any diameter is the same.
∴ Ix = Iy= 1/4 MR2 (Given)
According to the theorem of perpendicular axes,
Iz = Ix + Iy = 2(1/4MR2) = 1/2 MR2
Let I be the MI of the disc about a tangent normal to the disc and passing through a point on its edge (i.e., a tangent perpendicular to its plane). According to the theorem of parallel axis,
I = ICM + Mh2
Here, ICM = Iz = 1/2 MR2 and h = R.
∴ I = 1/2 MR2 + MR2 = 3/2 MR2
which is the required expression.