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Home/Electricity & Magnetism/Electric Dipole Field (2D)

Electric Dipole Field (2D)

±q on axis: V heatmap, equipotentials, E field lines; formulas.

Dipole ±q

0.22
1
32

Fixed on-axis dipole: +q at (−a, 0), −q at (+a, 0). Equipotentials are contour levels of the Coulomb potential (marching squares on a grid; singularities near charges are masked in the color scale).

Shortcuts

  • •Toggle heatmap vs lines to compare patterns
  • •Separation sets dipole arm 2a on the x-axis

Measured values

Dipole moment |p| ∝ 2aq0.2200 (sim)
V range (grid, masked)-23.37 … 23.37

About this model

A fixed two-charge dipole on the x-axis uses the Coulomb superposition V = Σ k qᵢ/rᵢ on a regular grid. A masked min/max range colors the heatmap away from singularities; equipotentials come from marching squares on that grid; field lines integrate forward along E from seeds near the positive charge until they reach the negative charge or the boundary.

Who it's for: Introductory electrostatics; complements the free-form Electric Field Visualizer with a formula-forward dipole preset.

Key terms

  • electric dipole
  • equipotential
  • field line
  • Coulomb potential
  • dipole moment

How it works

This page is dedicated to a pure dipole in 2D: two point charges +q and −q on the x-axis. The scalar potential V adds 1/r contributions; electric field lines follow E (perpendicular to equipotentials). Compare with the general Electric Field lab where you place arbitrary charges.

Key equations

V(r) = Σᵢ k qᵢ / |r − rᵢ|
E = −∇V (field lines tangent to E)
Far from origin: V ∝ (p·r̂)/r² , |p| = 2aq

Frequently asked questions

Why do contours look jagged near the charges?
The potential diverges at point charges; the visualization masks grid points very close to each charge when setting the color scale, and contour segments are piecewise linear on a finite grid.
How does this differ from the general electric field page?
That sandbox lets you place many charges interactively. Here the geometry is locked to a textbook ±q dipole so the text can quote standard dipole-field vocabulary and far-field behavior.