Let M be the mass of a thin ring of radius R. Let /CM be the moment of inertia (MI) of the ring about its transverse symmetry axis. Then,
ICM = MR … (1)
(1) MI about a diameter : Let x- and y-axes be along two perpendicular diameters of the ring as shown in below figure. Let Ix , Iy and Iz be the moments of inertia of the ring about the x, y and z axes, respectively.

Both Ix and Iy represent the moment of inertia of the ring about its diameter and, by symmetry, the MI of the ring about any diameter is the same.
∴ Ix = Iy ….. (2)
Also, Iz being the MI of the ring about its transverse symmetry axis,

Radius of gyration : The radius of gyration of the ring for rotation about its diameter is

(2) MI about a tangent in its plane: Let I be its MI about an axis in plane of the ring, i.e., parallel to a diameter, and tangent to it. Here, h = R and
ICM = Ix = \(\frac{1}2\) MR2 .
By the theorem of parallel axis,
= \(\frac{1}2\) MR2 + MR2 = \(\frac{3}2\) MR2 ....(7)

Radius of gyration : The radius of gyration of the ring for rotation about a tangent its olane is
