(d) An electric dipole is a pair of equal and opposite charges $q$ and $- q$ separated by some distance $2a.$ Its dipole moment vector $\overrightarrow{p}$ has magnitude $2qa\ $and is in the direction of the dipole axis from $- q$ to $q$
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The electric field due to a dipole at a point $p$ is
$E = \frac{p}{4\pi\varepsilon_{0}}\frac{\sqrt{3\cos^{2}{\theta + 1}}}{r^{3}}(r > > a)$
The electric dipole potential falls off at large distance, as $\frac{1}{r^{2}}$ not as $\frac{1}{r}$, characteristic of the potential due to a single charge.
In a uniform electric field $\overrightarrow{E},$ a dipole experiences a torque $\overrightarrow{\tau}$ given by $\overrightarrow{\tau} = \overrightarrow{p} \times \overrightarrow{E}$ but experiences no net force