textbf{Step 1:} Use the conservation of volume to find the relationship between the radius of the large drop ($R$) and the radius of the small drops ($r$):
\[ 1000 \cdot \frac{4}{3}\pi r^3 = \frac{4}{3}\pi R^3 \]
textbf{Step 2:} Solve for $R$ in terms of $r$:
\[ R^3 = 1000r^3 \implies R = 10r \]
textbf{Step 3:} Calculate the initial surface energy ($E_i$) of 1000 small drops:
\[ E_i = 1000 \cdot (4\pi r^2 \sigma) \]
textbf{Step 4:} Calculate the final surface energy ($E_f$) of the single large drop:
\[ E_f = 4\pi R^2 \sigma = 4\pi (10r)^2 \sigma = 100 \cdot (4\pi r^2 \sigma) \]
textbf{Step 5:} Find the ratio of final surface energy to initial surface energy:
\[ \frac{E_f}{E_i} = \frac{100 \cdot (4\pi r^2 \sigma)}{1000 \cdot (4\pi r^2 \sigma)} = \frac{100}{1000} = \frac{1}{10} \]