The angular velocity of a body changes from ω1 to ω2 without applying a torque but changing moment of inertia. The ratio of corresponding radii of gyration
As the torque applied on the given body is zero, we can conserve its angular momentum.
i.e., L1−L2
⇒I1ω1=I2ω2
(MK21)ω1=(MK22)ω2
⇒ K1K2=√ω2ω1=√ω2:√ω1