An electric dipole consists of two electric charges of equal magnitude and opposite sign. If the charges are $q$ and $-q$ and are located at a distance $d$ from each other, then the electric field $E$ at the point $P$ in the figure is
$$E=\frac{q}{D^{2}}-\frac{q}{(D+d)^{2}}$$
By expanding this expression for $E$ as a series in powers of $d / D,$ show that $E$ is approximately proportional to 1$/ D^{3}$ when $P$ is far away from the dipole.