Electric potential at an equatorial point of a small dipole with dipole moment $P$ ($r$, distance from the dipole) is
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(a) Electric potential at equatorial point of a small dipole moment $=P(\text { at } r)$
As we have learned,
if, $r>>1$
$E_{a x i}=\frac{1}{4 \pi \epsilon_{0}} \frac{2 P}{r^{3}}$
$V_{a x i}=\frac{1}{4 \pi \epsilon_{0}} \frac{P}{r^{2}}$
where,
angle between $E_{a x i}$ and $P$ will be $0$
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