1. Let the side of the equilateral triangle be $r$. The fourth particle of charge $3q$ is placed at the midpoint of one side.
2. Distance from the two adjacent charges = $r/2$, force magnitude due to each =
\[
F_\text{adj} = k \frac{(3q) q}{(r/2)^2} = 12 \, k \frac{q^2}{r^2} = 12F \quad (\text{since } F = k q^2 / r^2)
\]
3. The directions of these two forces are along the lines joining the fourth particle to the adjacent vertices. They form a $180^\circ$ angle (opposite directions along the line joining the two vertices). Net force along that line = $12F - 12F = 0$? Wait, vector addition carefully: forces are symmetric, horizontal components cancel, vertical components add: $F_\text{adj,net} = 12 F \sin 60^\circ = 12F \cdot \sqrt{3}/2 = 6\sqrt{3} F$.
4. Force from the third vertex (opposite corner): distance $r_\text{opposite} = \frac{\sqrt{3}}{2} r$, force magnitude =
\[
F_\text{opp} = k \frac{3q \cdot q}{(\frac{\sqrt{3}}{2} r)^2} = \frac{12}{3} F = 4F
\]
5. This force acts horizontally toward the midpoint. Vector sum of vertical and horizontal components gives
\[
F_\text{net} = \sqrt{(6F \cdot 0.5?)^2 + 4F^2} = \sqrt{3} F
\]