Step 1: Understanding the Question:
A child stands at the center of a friction-free turntable system rotating at an initial velocity. The initial rotational kinetic energy is $K$. When the child extends their arms outward, the total moment of inertia of the system doubles ($I_2 = 2I_1$). We need to find the new rotational kinetic energy $K_2$.
Step 2: Key Formula or Approach:
Because there are no external forces or torques acting on the system ($\tau_{\text{ext}} = 0$), the total angular momentum $L$ is perfectly conserved:
$$L = I_1 \omega_1 = I_2 \omega_2 = \text{constant}$$
The rotational kinetic energy can be expressed in terms of angular momentum and the moment of inertia using the formula:
$$K = \frac{L^2}{2I}$$
This shows that kinetic energy is inversely proportional to the moment of inertia: $K \propto \frac{1}{I}$.
Step 3: Detailed Explanation:
Let's write down the ratio of the initial and final kinetic energies using our proportional relationship:
$$\frac{K_2}{K_1} = \frac{I_1}{I_2}$$
We are given that the new moment of inertia is double the original value ($I_2 = 2I_1$). Substituting this into the ratio gives:
$$\frac{K_2}{K} = \frac{I_1}{2I_1}$$
The individual moment of inertia terms $I_1$ cancel out perfectly:
$$\frac{K_2}{K} = \frac{1}{2} \implies K_2 = \frac{K}{2}$$
Step 4: Final Answer:
The rotational kinetic energy of the system becomes $\frac{K}{2}$, which corresponds to option (A).