Let the charges be placed at the three corners of a square of side $l$, with point $O$
at the fourth corner.
The distance of each charge from point $O$ is:
\[
r = \sqrt{l^2 + l^2} = l\sqrt{2}
\]
Hence,
\[
r^2 = 2l^2
\]
Electric field due to one charge $q$ at $O$:
\[
E = \frac{1}{4\pi\epsilon_0}\frac{q}{2l^2}
\]
Two charges are placed symmetrically such that their horizontal components cancel
and their vertical components add.
Resultant field due to these two charges:
\[
E_1 = 2E\cos45^\circ
= 2\left(\frac{1}{4\pi\epsilon_0}\frac{q}{2l^2}\right)\frac{1}{\sqrt{2}}
= \frac{1}{4\pi\epsilon_0}\frac{\sqrt{2}q}{2l^2}
\]
The third charge produces a field directly opposite to $E_1$ with magnitude:
\[
E_2 = \frac{1}{4\pi\epsilon_0}\frac{q}{2l^2}
\]
Therefore, net electric field at point $O$:
\[
E = E_1 - E_2
= \frac{1}{4\pi\epsilon_0}\frac{q}{2l^2}(\sqrt{2}-1)
\]
Since two such perpendicular contributions exist, total magnitude becomes:
\[
E = \frac{1}{4\pi\epsilon_0}\frac{q}{2l^2}(2\sqrt{2}-1)
\]