Suppose a rigid body is made of n particles of masses m1, m2, m3, ......, mn and their distances from the axes of rotation YY' are r1, r2, r3, .........., rn respectively. If a1, a2, a3, ......., an are linear accelerations of the particles, then forces acting on the particles,


If the body is rotating with the angular acceleration α, then
F1 = m1a = m1r1α (because a1 = r1α)

∵ Torque = force x normal distance from the axis of rotation
or τ = F x r
or τ = mrα x r = mr2α
∴ τ1 = m1r12α; τ2 = m2r22α; ....., τn = mnrn2α
∴ If all these torque are in the same direction then net torque acting on the body,
τ = τ1 + τ2 + τ3 + .......+ τn
= m1r12α + m2r22α + m3r32α + ..... + mnrn2α
= (m1r12 + m2r22 + m3r32 + ........ + mnrn2)α
\( = \sum_{i = 1}^n\ m_ir_i^2\ .\ \alpha\)
or \(\tau = I\alpha\)
i.e., Torque = Moment of inertia x Angular acceleration,
If α = 1 rad.s-1, then τ = I
i.e., "Momentum of inertia of a body about a given axis of rotation is equivalent to torque which can produce unit angular acceleration in the body."