The electric potential \( V \) generated by a point charge \( q \) at a distance \( r \) is given by:
\[ V = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q}{r} \]
The total electric potential at the point is the superposition of the potentials from individual charges:
\[ V_{\text{total}} = V_1 + V_2 = \frac{1}{4\pi\varepsilon_0} \left( \frac{q_1}{r_1} + \frac{q_2}{r_2} \right) = 0 \]
Substituting known values:
\[ \frac{1}{4\pi\varepsilon_0} \left( \frac{2 \times 10^{-9} \, \text{C}}{2 \, \text{m}} + \frac{q_2}{8 \, \text{m}} \right) = 0 \]
Simplifying the equation:
\[ 1 \times 10^{-9} + \frac{q_2}{8} = 0 \]
Solving for \( q_2 \):
\[ \frac{q_2}{8} = -1 \times 10^{-9} \, \text{C} \]
\[ q_2 = -8 \times 10^{-9} \, \text{C} \]
The unknown charge is: \( q_2 = -8 \, \text{nC} \), situated at \( (0, 0, -6) \, \text{m} \)