Step 1: State the formula for the force between two charges with an intervening medium.
The force between two point charges $q_1$ and $q_2$ separated by a distance $r$ is $F = \frac{1}{4\pi\epsilon} \frac{q_1 q_2}{r^2}$.
When a medium of dielectric constant $K$ fills a thickness $t$ between the charges (with a total distance $r$), the effective distance in the denominator of the force is changed from $r$ to $r_{eff}$.
\[
F' = \frac{1}{4\pi\epsilon_0} \frac{q_1 q_2}{[r_{eff}]^2}.
\]
The effective distance for the force calculation is given by:
\[
r_{eff} = (r-t) + t\sqrt{K}.
\]
The force can be written as $F' = F_{air} \frac{r^2}{[r_{eff}]^2}$.
Step 2: Apply the given condition to find the effective distance.
The initial force in air is $F_{air} = F$.
The final force is $F' = \frac{F}{2.56}$.
The distance $r$ remains the same. The ratio of the forces is $\frac{F_{air}}{F'} = \frac{[r_{eff}]^2}{r^2} = 2.56$.
\[
\frac{r_{eff}}{r} = \sqrt{2.56} = 1.6.
\]
So, $r_{eff} = 1.6r$.
Step 3: Use the given thickness of the medium.
The thickness of the medium is $t = 30%$ of the total distance $r$.
\[
t = 0.3r.
\]
Step 4: Substitute the effective distance formula and solve for K.
We have $r_{eff} = 1.6r$ and $t = 0.3r$.
Substitute these into the effective distance formula:
\[
r_{eff} = (r-t) + t\sqrt{K}.
\]
\[
1.6r = (r - 0.3r) + 0.3r\sqrt{K}.
\]
\[
1.6r = 0.7r + 0.3r\sqrt{K}.
\]
Divide by $r$:
\[
1.6 = 0.7 + 0.3\sqrt{K}.
\]
\[
0.3\sqrt{K} = 1.6 - 0.7 = 0.9.
\]
\[
\sqrt{K} = \frac{0.9}{0.3} = 3.
\]
Squaring both sides gives the dielectric constant:
\[
\boxed{K = 9}.
\]