Step 1: Understanding the Concept:
No external torque acts, so angular momentum is conserved. The second ring starts at rest and then moves with the first, so energy is lost as friction heat.
Step 2: Find the final angular velocity:
\(I\omega=(I+I)\omega'\), so \(\omega'=\dfrac\omega2\).
Step 3: Find the kinetic energies:
Initial: \(K_i=\dfrac12I\omega^2\). Final: \(K_f=\dfrac12(2I)\left(\dfrac\omega2\right)^2=\dfrac14I\omega^2\).
Step 4: Find the loss:
\(K_i-K_f=\dfrac12I\omega^2-\dfrac14I\omega^2=\dfrac14I\omega^2\). Option C.
Step 5: Why the other options are wrong.
\(I\omega^2\) and \(\dfrac{I\omega^2}{2}\) are bigger than or equal to the initial energy, which cannot be lost. \(\dfrac{I\omega^2}{8}\) comes from halving the correct loss.
Final Answer:
The loss in kinetic energy is I omega^2 / 4.
\[ \boxed{\text{(C) }\dfrac{I\omega^2}{4}} \]