The electrostatic potential due to an electric dipole at a distance ’ $r$ ’ varies as:
(1) $\mathrm{r}$
(2) $\frac{1}{r^{2}}$
(3) $\frac{1}{r^{3}}$
(4) $\frac{1}{r}$
$V=\frac{k P \cos \theta}{r^{2}}$
$&$ can also checked dimensionally
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