Step 1: Electric potential of a dipole.
The electric potential at a point on the axial line of an electric dipole is given by:
\[
V = \frac{1}{4 \pi \epsilon_0} \frac{2p \cos \theta}{r^2}
\]
where:
- \( V \) is the electric potential,
- \( p \) is the dipole moment (\( p = q \times 2a \), where \( q \) is the charge and \( 2a \) is the separation between the charges),
- \( r \) is the distance from the center of the dipole to the point where the potential is being calculated,
- \( \theta \) is the angle between the dipole axis and the position vector of the point,
- \( \epsilon_0 \) is the permittivity of free space.
Step 2: Electric potential along the axial line.
For points along the axial line, \( \theta = 0 \), so \( \cos 0 = 1 \), and the electric potential simplifies to:
\[
V = \frac{1}{4 \pi \epsilon_0} \frac{2p}{r^2}
\]
Step 3: Conclusion.
The electric potential at a point on the axial line of an electric dipole is:
\[
V = \frac{1}{4 \pi \epsilon_0} \frac{2p}{r^2}
\]