Electric Dipole Calculator

Calculate dipole field and potential energy at distance r and angle θ

Parameters

C·mⓘ
mⓘ
°ⓘ
Show Trail

Controls

xⓘ

Calculated Values

Field (approx):
17980.00;N/C17980.00;N/C
Potential Energy:
−0.00;J-0.00;J

Examples

p = 10⁻⁹ C·m, r = 0.1 m

On-axis field estimate.

    p = 2×10⁻⁹ C·m, θ = 60°

    Energy in external field context.

      Visualization

      Electric Dipole — Field, Torque, and Energy

      An electric dipole consists of +q and −q separated by distance d. Dipole moment p⃗ = q d⃗ points from − to +, SI unit C·m.

      Far from the dipole (r >> d), field falls as 1/r³ (faster than point charge 1/r²). On axis: E ≈ 2kp/r³; on equatorial line: E ≈ kp/r³.

      Torque in uniform field: τ⃗ = p⃗ × E⃗, magnitude τ = pE sinθ. Dipole tends to align with E (θ → 0 minimizes energy).

      Potential energy U = −p⃗·E⃗ = −pE cosθ. Stable equilibrium at θ = 0 (aligned); unstable at θ = π.

      Polar molecules (H₂O, HCl) have permanent p; nonpolar molecules can gain induced dipole in external E (polarization).

      Dipole radiation: accelerating or oscillating dipoles emit EM waves — basis of antenna theory at λ >> dipole size.

      Key Concepts

      • p = qd — dipole moment
      • E ∝ 1/r³ at large r
      • τ = pE sinθ — torque
      • U = −pE cosθ — potential energy
      • Stable when p parallel to E
      • Net charge zero, field nonzero

      Real-World Applications

      • Polar solvents and dielectrics
      • Dipole antennas (radio/TV)
      • Liquid crystal displays
      • Molecular orientation in E fields
      • Class 12 dipole field derivations

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      Physics Equations

      Dipole Moment:
      p=qdp = qd
      Potential Energy:
      U=−pEcos⁡θU = -pE\cos\theta

      Step-by-Step Solution

      See how the main results are calculated.

      1

      Step 1: Dipole Moment

      Equation:

      p=qdp = q d

      Result:

      p=1.0000e−9 C\cdotpmp = 1.0000e-9 \text{ C·m}

      Explanation:

      Vector from −q to +q, magnitude q×separation. Net charge of ideal dipole is zero.

      2

      Step 2: Geometry — Distance and Angle

      Field point at distance r from center, angle θ from dipole axis.

      Calculation:

      r=0.1 m,θ=0°=0.0000 radr = 0.1 \text{ m}, \quad \theta = 0° = 0.0000 \text{ rad}

      Explanation:

      Valid for r >> dipole size d (point dipole approximation).

      3

      Step 3: On-Axis Field Reference

      Equation:

      Eaxis=2kpr3E_{axis} = \frac{2kp}{r^3}

      Calculation:

      Eaxis=2×(8.99×109)×1.0000e−90.13=1.7980e+4 N/CE_{axis} = \frac{2 \times (8.99 \times 10^9) \times 1.0000e-9}{0.1^3} = 1.7980e+4 \text{ N/C}

      Explanation:

      On-axis field is twice equatorial field at same r for ideal dipole.

      4

      Step 4: Field at Angle θ

      Evaluate field magnitude at observation angle θ from dipole axis.

      Calculation:

      E≈1.7980e+4 N/CE \approx 1.7980e+4 \text{ N/C}

      Result:

      E ≈ 1.7980e+4 N/C

      Explanation:

      General point-dipole field components combine to this magnitude at angle θ.

      5

      Step 5: Potential Energy in External Field

      Equation:

      U=−p⃗⋅E⃗=−pEcos⁡θU = -\vec{p} \cdot \vec{E} = -pE\cos\theta

      Calculation:

      U≈−8.9900e−6 JU \approx -8.9900e-6 \text{ J}

      Result:

      U ≈ -8.9900e-6 J

      Explanation:

      Minimum U at θ = 0° (aligned); maximum at θ = 180°; U = 0 at θ = 90°.

      6

      Step 6: Torque Tending to Align Dipole

      Equation:

      τ=pEsin⁡θ\tau = pE\sin\theta

      Calculation:

      τ≈0.0000e+0 N\cdotpm (magnitude)\tau \approx 0.0000e+0 \text{ N·m (magnitude)}

      Explanation:

      Torque rotates dipole until p aligns with E (stable equilibrium at θ = 0 in uniform field).

      Frequently Asked Questions (FAQ)

      Why 1/r³ for dipole?

      At large r, +q and −q fields nearly cancel; leading term is dipole contribution ∝ p/r³.

      Field on equatorial vs axial line?

      Different geometry factors but both ∝ 1/r³; axial is 2× equatorial for same r (ideal point dipole).

      Can a dipole feel force in uniform E?

      Pure uniform E: torque only. Non-uniform E can exert net force (F ∝ ∇(p·E)).

      Induced vs permanent dipole?

      Permanent: fixed p. Induced: p from electron shift in external E (polarization).

      Energy at θ = 90°?

      U = 0 (cos 90° = 0) — neither max nor min; unstable equilibrium in 2D rotation.

      Practice MCQs

      1. Stable equilibrium angle for dipole in uniform E:
      2. Compared to point charge field at large r, dipole field E falls as:
      3. Dipole moment p has units:
      4. Maximum torque on dipole in field E occurs at:
      5. Net charge of an ideal dipole is:
      6. Water is a good solvent partly because it is: