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Electric field due to an electric dipole on its equatorial line

E = kp/r³

p is the dipole moment and r ≫ a is the distance from the centre along the perpendicular bisector.

Derivation

  1. Each charge is √(r² + a²) away and gives a field of size kq/(r² + a²).
  2. The components along the bisector cancel; the components parallel to the axis add.
  3. E = 2 × kq/(r² + a²) × a/√(r² + a²) = kp/(r² + a²)^(3/2) ≈ kp/r³, opposite to p.

Points to remember

  • Direction is opposite to the dipole moment.
  • E(axial) : E(equatorial) = 2 : 1.

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Questions students ask

What is the electric field due to an electric dipole on its equatorial line?

E = kp/r³. p is the dipole moment and r ≫ a is the distance from the centre along the perpendicular bisector.

How do you derive the electric field due to an electric dipole on its equatorial line?

Each charge is √(r² + a²) away and gives a field of size kq/(r² + a²). The components along the bisector cancel; the components parallel to the axis add. E = 2 × kq/(r² + a²) × a/√(r² + a²) = kp/(r² + a²)^(3/2) ≈ kp/r³, opposite to p.

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