(d) Electric field due to an electric dipole at axial point
$E_{axial} = \frac{2kpr}{\left( r^{2} - l^{2} \right)^{2}}$
$If\ r \gg l,\ E_{a} = \frac{1}{4\pi\varepsilon_{0}}\frac{2p}{r^{3}}$
$\Longrightarrow E \propto \frac{1}{r^{3}}$
(directed from –q to +q)