Electrostatic Potential and Capacitance

Physics · Class 12

Lesson 2 of 13 · 7 min

Potential due to a dipole

NCERT §2.4

Meera's teacher hands her a plastic stick with two small beads 2 cm apart, one at +10 nC and one at −10 nC: a dipole you can hold. Where around it is the potential positive, where negative, and where zero?

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In short

A dipole is charges +q and −q a distance 2a apart; its dipole moment p = q × 2a points from −q to +q.

Far from the dipole (r ≫ a), V = p cos θ/(4πε₀r²), where θ is the angle between p and the line to the point. In vector form V = p·r̂/(4πε₀r²).

On the axis (θ = 0° or 180°) V = ±p/(4πε₀r²); on the equatorial plane (θ = 90°) V = 0 everywhere.

Dipole potential falls as 1/r², faster than a single charge's 1/r, because the two opposite charges nearly cancel at a distance.

The dipole potential depends on direction as well as distance: it is not spherically symmetric, unlike a point charge's.

Zero potential on the equatorial plane does not mean zero field there: E on the equator is p/(4πε₀r³), pointing opposite to p.

Potential due to a dipole | Electrostatic Potential and Capacitance | Lumi Learn