(b) Here total electrostatic potential energy is zero
$ie,\ \ \frac{- \mathcal{Q}_{0}q}{l} - \frac{q\mathcal{Q}_{0}}{l} + \frac{q^{2}}{\sqrt{2l}} = 0$
On solving,
$\mathcal{Q}_{0} = \frac{q}{2\sqrt{2}} = \frac{2q}{\sqrt{32}}$
[image:2_image135.emf]