Step 1: Understanding the Concept:
The dancer's rotational kinetic energy depends on both the moment of inertia \(I\) and the angular velocity \(\omega\). No external torque acts, so angular momentum \(I\omega\) stays constant.
Step 2: Key Formula or Approach:
\[ K = \frac12I\omega^2 \]
Step 3: Detailed Explanation:
Initially \(K = \dfrac12I\omega^2\).
After stretching the arms, \(I' = 3I\) and \(\omega' = \dfrac\omega3\). Check that the angular momentum is conserved: \(I'\omega' = 3I\cdot\dfrac\omega3 = I\omega\). It is.
New kinetic energy:
\[ K' = \frac12(3I)\left(\frac\omega3\right)^2 = \frac12\cdot3I\cdot\frac{\omega^2}{9} = \frac13\left(\frac12I\omega^2\right) = \frac K3 \]
The kinetic energy decreases, because the dancer's arm muscles do negative work when stretching out against the spin. Option (A) K/6, (C) 3K and (D) 6K do not follow from this calculation.
Final Answer:
The new kinetic energy is \(\dfrac K3\), option (B).
\[ \boxed{\frac{K}{3} \text{ (B)}} \]