By observing the figure
Force acting on charge \(q\) at \(A\) due to charge \(q\) at \(B\) is \(F_{12}\) along \(\mathit{BA}\) as both charges are of same nature therefore repulsive in nature.
Force acting on charge \(q\) at \(A\) due to charge \(-q\) at \(C\) is \(F_{13}\) along \(\mathit{AC}\) as both charges are opposite in nature therefore attracts each other.
By the law of parallelogram, the total force \(F_1\) on the charge \(q\) at \(A\) can be found as,
\(F_1=Fȓ_1\)
where as \(ȓ_1\) is a unit vector along \(\mathit{BC}\) which is at an angle of \(120^{\circ}\) from \(x\)- axis .
The force of attraction or repulsion for each pair of charges \((\)either \(\mathit{AB}\) or \(\mathit{BC}\) or \(\mathit{CA})\) has the same magnitude and therefore,
\(F=\frac 1{4\pi \varepsilon _0}\frac{q^2}{l^2}\)
where the magnitude of charge is \(q\) and the distance between each pair is \(l\) .
The total force \(F_2\) on charge \(q\) at \(B\) is therefore \(F_2=Fȓ_2\) , where \(ȓ_2\) is a unit vector along \(\mathit{AC}\) .
And the total force on charge \(-q\) at \(C\) is \(F_3=\sqrt 3F\widehat n\) , where \(\widehat n\) is the unit vector along the direction bisecting the \({\angle}\mathit{BCA}\) .