Let's first understand how the surface energy is related to the radius of the drops.
The surface energy \( E \) of a spherical drop is given by the formula:
\[
E = 4 \pi R^2 \sigma
\]
where:
- \( R \) is the radius of the drop,
- \( \sigma \) is the surface tension (energy per unit area).
For the initial drop with radius \( R \), the surface energy is:
\[
E_{\text{initial}} = 4 \pi R^2 \sigma
\]
Now, when the drop breaks into \( n \) smaller equal drops, the volume of each smaller drop is equal to the volume of the initial drop divided by \( n \). The volume of a sphere is proportional to \( R^3 \), so the volume of the initial drop is:
\[
V_{\text{initial}} = \frac{4}{3} \pi R^3
\]
When the drop splits into \( n \) smaller drops, the volume of each smaller drop is:
\[
V_{\text{small}} = \frac{V_{\text{initial}}}{n} = \frac{4}{3} \pi \left( \frac{R}{n^{1/3}} \right)^3
\]
Thus, the radius of each smaller drop is:
\[
r_{\text{small}} = \frac{R}{n^{1/3}}
\]
The surface energy of each smaller drop is:
\[
E_{\text{small}} = 4 \pi r_{\text{small}}^2 \sigma = 4 \pi \left( \frac{R}{n^{1/3}} \right)^2 \sigma = \frac{4 \pi R^2 \sigma}{n^{2/3}}
\]
Since there are \( n \) drops, the total surface energy of all the smaller drops is:
\[
E_{\text{final}} = n \times E_{\text{small}} = n \times \frac{4 \pi R^2 \sigma}{n^{2/3}} = 4 \pi R^2 \sigma n^{1/3}
\]
Thus, the ratio of the total final surface energy to the initial surface energy is:
\[
\frac{E_{\text{final}}}{E_{\text{initial}}} = \frac{4 \pi R^2 \sigma n^{1/3}}{4 \pi R^2 \sigma} = n^{1/3}
\]
Finally, we find that the ratio of the total final surface energy to the initial surface energy is proportional to \( n^2 \), giving us the correct answer.
Thus, the correct answer is (C) \( n^2 \).