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IO = mr2
IO = ∑miri2
If we think of a rigid body as a collection of infinitesimally small particles, the mass moment of inertia becomes the integral form of the mass moment of inertia for a system of particles.
IO = ∫ri2 dm
It is often the case that a body’s mass moment of inertia with respect to an axis is expressed in terms of its radius of gyration (k) with respect to that axis.
I = mk2