Step 1: Understanding the concept of surface charge density.
Surface charge density (\( \sigma \)) is the charge per unit surface area. It is
given by:
\[
\sigma = \frac{Q}{A}
\]
where \( Q \) is the charge and \( A \) is the surface area of the droplet.
Step 2: Total charge conservation.
Since all 27 droplets have the same charge, and they coalesce to form a single larger droplet, the total charge remains the same.
Step 3: Relating the radius of the droplets.
The total volume is conserved in the process. The volume of a sphere is
given by:
\[
V = \frac{4}{3} \pi r^3
\]
For 27 small droplets of radius \( r = 3 \, \text{mm} \), the total volume of the small droplets is:
\[
V_{\text{small}} = 27 \times \frac{4}{3} \pi r^3
\]
For the large droplet, the radius is \( R \), and the volume is:
\[
V_{\text{large}} = \frac{4}{3} \pi R^3
\]
Since the total volume is conserved, we have:
\[
V_{\text{small}} = V_{\text{large}} \quad \Rightarrow \quad 27 \times r^3 = R^3
\]
This gives:
\[
R = 3r
\]
Step 4: Finding the ratio of surface charge densities.
The surface area of a sphere is
given by:
\[
A = 4 \pi r^2
\]
Thus, the surface area of the small droplet is \( A_{\text{small}} = 4 \pi r^2 \) and the surface area of the large droplet is \( A_{\text{large}} = 4 \pi (3r)^2 = 36 \pi r^2 \).
Now, the surface charge densities are:
\[
\sigma_{\text{small}} = \frac{Q}{A_{\text{small}}} = \frac{Q}{4 \pi r^2}, \quad \sigma_{\text{large}} = \frac{Q}{A_{\text{large}}} = \frac{Q}{36 \pi r^2}
\]
Thus, the ratio of surface charge densities is:
\[
\frac{\sigma_{\text{small}}}{\sigma_{\text{large}}} = \frac{\frac{Q}{4 \pi r^2}}{\frac{Q}{36 \pi r^2}} = 9
\]
Therefore, the ratio is \( \text{3:1} \), not \( 9:1 \).
Thus, the correct answer is
(C) 3 : 1.