(N/A) $(i)$ The $Cs^{+}$ ions are situated at the corners of a cube and the $Cl^{-}$ ion is at the centre. Due to the symmetry of the cube, the electric field produced by each $Cs^{+}$ ion at the centre is equal in magnitude and directed away from the corner towards the opposite corner. These fields cancel each other out in pairs. Therefore, the net electric field at the centre is $0 \, N/C$.
$(ii)$ Let $\vec{E}_{total}$ be the electric field due to all eight $Cs^{+}$ ions at the centre, which is $0$. If one $Cs^{+}$ ion at corner $A$ is removed, the new electric field $\vec{E}'$ at the centre is given by $\vec{E}' + \vec{E}_{A} = 0$, where $\vec{E}_{A}$ is the field due to the $Cs^{+}$ ion at $A$. Thus, $\vec{E}' = -\vec{E}_{A}$.
The distance $r$ from a corner to the centre of a cube of side $a = 0.40 \, nm$ is half the body diagonal: $r = \frac{\sqrt{3}a}{2} = \frac{\sqrt{3} \times 0.40 \times 10^{-9}}{2} = 0.20\sqrt{3} \times 10^{-9} \, m \approx 3.464 \times 10^{-10} \, m$.
The magnitude of the electric field due to one $Cs^{+}$ ion at the centre is $E_{A} = \frac{k e}{r^2} = \frac{9 \times 10^9 \times 1.6 \times 10^{-19}}{(0.20\sqrt{3} \times 10^{-9})^2} = \frac{14.4 \times 10^{-10}}{12 \times 10^{-20}} = 1.2 \times 10^{10} \, N/C$.
The force on the $Cl^{-}$ ion (charge $-e$) due to the remaining seven $Cs^{+}$ ions is $\vec{F} = (-e) \vec{E}' = (-e) (-\vec{E}_{A}) = e \vec{E}_{A}$.
The magnitude of the force is $F = e E_{A} = (1.6 \times 10^{-19}) \times (1.2 \times 10^{10}) = 1.92 \times 10^{-9} \, N$, directed towards the empty corner $A$.