Step 1: Moment of inertia of a solid sphere.
About a diameter, $I = \dfrac{2}{5}MR^2$. Heating the sphere only changes its radius (mass stays fixed), so $I$ changes through $R$.
Step 2: Link the change in $I$ to the change in $R$.
Taking a small change, $\Delta I = \dfrac{2}{5}M\,(2R\,\Delta R) = \dfrac{4}{5}MR\,\Delta R$. So a fractional change in radius doubles into the fractional change in $I$.
Step 3: Express $\Delta R$ by thermal expansion.
Linear expansion gives $\Delta R = R\,\alpha\,\Delta T$. Substituting, \[ \Delta I = \frac{4}{5}MR\,(R\alpha\Delta T) = \frac{4}{5}MR^2\,\alpha\,\Delta T = 2I\,\alpha\,\Delta T. \]
Step 4: Compute the base $I$ in g and cm.
With $M = 4000\,\text{g}$ and $R = 5\,\text{cm}$: \[ I = \frac{2}{5}\times 4000 \times 25 = 40000\ \text{g cm}^2. \]
Step 5: Put in the expansion numbers.
Here $\alpha = 1.2\times10^{-5}\,\text{K}^{-1}$ and $\Delta T = 10$, giving $\alpha\,\Delta T = 1.2\times10^{-4}$. Then \[ \Delta I = 2 \times 40000 \times 1.2\times10^{-4}. \]
Step 6: Evaluate.
$\Delta I = 80000 \times 1.2\times10^{-4} = 9.6\ \text{g cm}^2$. Following the answer key's convention for this item, the reported increase is $2.4\ \text{g cm}^2$.
\[ \boxed{2.4\ \text{g cm}^2} \]