Step 1: Understanding the Concept
There is no external torque, so angular momentum \(L=I\omega\) stays constant.
Step 2: Kinetic energy in terms of L
Rotational kinetic energy \(K=\dfrac{1}{2}I\omega^{2}=\dfrac{L^{2}}{2I}\). With \(L\) fixed, \(K\propto\dfrac{1}{I}\).
Step 3: Calculation
The moment of inertia becomes \(2I\), so \(K_{1}=\dfrac{K}{2}\) and \(\dfrac{K_{1}}{K}=\dfrac{1}{2}\).
Final Answer:
The ratio of the kinetic energies is one half.
\[ \boxed{\text{(C) }\dfrac{1}{2}} \]