A rigid body can be supposed to be made of many small particles. The moment of inertia of the rigid body is obtained by the sum of moment of inertias of individual particles i.e.,
I = I1 + I2 + I3 + ......... + In


where m1, m2, m3, ....., mn are the masses of the particles of rigid body and their distances from the axis of rotation are r1, r2, r3, ...., rn respectively as shown in fig.

Moment of inertia of a rigid body can be obtained by
I = m1r12 + m2r22 + m3r32 + ..... + mnrn2
This method is pure theoretical but practically it is very difficult, say rather impossible. Therefore to obtain moment of inertia of a rigid body, we consider a point in the body where all the mass of the body is considered centralized such that the square of its distance from the axis of rotation when multiplied with the mass of the body, then moment of inertia is obtained. This distance is called the ‘radius of gyration’ and it is denoted by K.
∴ I = MK2
or \(K = \sqrt{\frac{I}{M}}\ ...(1)\)
If the body is supposed to be made of n particles, then
I = m1r12 + m2r22 + m3r32 + .......... + mnrn2
And M = m1 + m2 + m3 + ....... + mn
\(\therefore\ K = \sqrt{\frac{m_1r_1^2 + m_2r_2^2 + ....+m_nr_n^2}{m_1 + m_2 + ...+m_n}}\ ...(2)\)
If mass of each particle be m, i.e.,
m1 = m2 = m3 = .......... = mn
Then M = m + m + .......... + m(n times)
or M = mn ..........(3)
