Using the conservation of volume, the volume of the big drop is equal to the sum of the volumes of the 1000 smaller drops:
\[
\frac{4}{3}\pi R^3 = 1000 \cdot \frac{4}{3}\pi r^3,
\]
where \( R \) is the radius of the large drop and \( r \) is the radius of each smaller drop.
Simplify:
\[
R^3 = 1000 \cdot r^3 \implies R = 10r.
\]
The surface energy of a sphere is proportional to its surface area. The initial energy (for 1000 small drops) is:
\[
E_i = 1000 \cdot 4\pi r^2.
\]
The final energy (for the large drop) is:
\[
E_f = 4\pi R^2 = 4\pi (10r)^2 = 100 \cdot 4\pi r^2.
\]
Thus, the ratio of the final to initial energy is:
\[
\frac{E_f}{E_i} = \frac{4\pi (10r)^2}{1000 \cdot 4\pi r^2} = \frac{1}{10}.
\]
Final Answer:
\[
\boxed{\frac{1}{10} \, \text{th}}.
\]