Potential Energy of a Dipole in an External Field

Physics · Electrostatic Potential And Capacitance · NEET

When an electric dipole (moment p) sits in a uniform external field E, its potential energy is U = -pE cosθ, where θ is the angle between p and E. Memory hook: "aligned = lowest, anti = highest" — U is most negative (-pE) when the dipole points along the field (θ = 0, stable) and most positive (+pE) when it points against it (θ = 180°, unstable). At θ = 90° the energy is zero, so we measure PE from the perpendicular position.
Dipole in a uniform field E: U = -pE cosθfield E-+pθ = 0°: U = -pE (stable, min)θtilted θ: U = -pE cosθtorque τ = pE sinθ turns it back
A dipole moment p in a uniform field E. Aligned (θ = 0°) gives the lowest energy U = -pE (stable); tilted by θ gives U = -pE cosθ, and a restoring torque τ = pE sinθ pulls it back toward alignment.

Your doubts, answered

Why is the potential energy of a dipole negative?

The minus sign in U = -pE cosθ just tells you the direction of the energy compared to the θ = 90° reference. When the dipole is aligned with the field (θ = 0), cosθ = 1, so U = -pE, a negative (minimum) value. Nature always pushes systems toward lowest energy, so the dipole is 'happy' and stable when aligned — that is why U is most negative there. It is not saying energy is 'missing'; it means work was released as the dipole turned into the field.

What exactly is θ in U = -pE cosθ?

θ is the angle between the dipole moment vector p (which points from the -q charge to the +q charge) and the external field E. It is NOT the angle with any wall or plate. Always draw the p arrow first, then measure how far it is tilted from E. θ = 0 means p points along E; θ = 180° means p points opposite to E.

Why do we take potential energy zero at 90° and not at 0°?

By convention we bring the dipole in from the θ = 90° (perpendicular) position because there the field does no net work while rotating the dipole into place (torque is balanced in a symmetric way). Putting U = 0 at 90° makes the formula clean: U = -pE cosθ, which gives -pE at 0° and +pE at 180°. This is the NCERT-chosen reference, so use it for NEET.

How is potential energy different from torque for a dipole?

Torque τ = pE sinθ is the turning effect that tries to rotate the dipole; it is largest at θ = 90° and zero at 0° and 180°. Potential energy U = -pE cosθ is the stored energy; it is lowest at 0° and highest at 180°. Torque is a vector (a cause of rotation); U is a scalar (a stored amount). Both come from the same p and E but answer different questions.

How do I find the change in PE when a dipole is rotated?

Use ΔU = U(θ₂) - U(θ₁) = -pE(cosθ₂ - cosθ₁) = pE(cosθ₁ - cosθ₂). This ΔU equals the work you must do to rotate it (against the field). Example: from θ₁ = 0° to θ₂ = 60°, ΔU = pE(cos0° - cos60°) = pE(1 - 0.5) = 0.5 pE.

⚠️ The NEET trap
Plugging into U = -pE cosθ and thinking that gives the work done, so writing work = -pE cos60° = -pE/2.
Work done to rotate equals the CHANGE in PE: W = ΔU = -pE(cosθ₂ - cosθ₁) = pE(cosθ₁ - cosθ₂). From 0° to 60°, W = pE(1 - 0.5) = +0.5 pE, a positive value.
🧠 U at one angle is not the work. Work always needs TWO angles: subtract final minus initial.

Real NEET questions

NEET 2025

An electric dipole with dipole moment 5 × 10⁻⁶ C·m is aligned with the direction of a uniform electric field of magnitude 4 × 10⁵ N/C. The dipole is then rotated through an angle of 60° with respect to the electric field. The change in the potential energy of the dipole is:

A · 1.2 J
B · 1.5 J
C · 0.8 J
D · 1.0 J
Solution: Start aligned, so θ₁ = 0°; rotated by 60°, so θ₂ = 60°. ΔU = -pE(cosθ₂ - cosθ₁) = -pE(cos60° - cos0°) = -pE(0.5 - 1) = 0.5 pE. Compute pE = (5 × 10⁻⁶)(4 × 10⁵) = 2 J. So ΔU = 0.5 × 2 = 1.0 J. Answer: (D).
NEET 2021

A dipole is placed in an electric field (as shown in the figure). In which direction will it move?

A · Towards the left as its potential energy will decrease
B · Towards the right as its potential energy will increase
C · Towards the left as its potential energy will increase
D · Towards the right as its potential energy will decrease
Solution: In a non-uniform field a dipole feels a net force pulling it toward the stronger-field region, because a system always moves so that its potential energy U = -p·E decreases (becomes more negative). Per the figure, that stronger-field side is to the right, so the dipole moves towards the right while its potential energy decreases. Answer: (D).

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Frequently asked

What is the formula for the potential energy of a dipole in a uniform field?

U = -pE cosθ, or in vector form U = -p·E, where p is the dipole moment, E is the field, and θ is the angle between them. It gives -pE at θ = 0° and +pE at θ = 180°.

At what angle is the potential energy of a dipole minimum?

At θ = 0°, when the dipole is aligned with the field. Then cosθ = 1 and U = -pE, the minimum (most negative) value. This is the stable equilibrium position.

What is the potential energy of a dipole at 90°?

Zero. At θ = 90°, cos90° = 0, so U = -pE(0) = 0. This perpendicular position is the chosen reference from which PE is measured.

Which position is stable and which is unstable for a dipole?

θ = 0° (aligned with E) is stable — lowest energy, torque restores it if disturbed. θ = 180° (anti-parallel to E) is unstable — highest energy, any small push turns it away.

Does a dipole have net force in a uniform field?

No. In a uniform field the two charges feel equal and opposite forces, so net force is zero — only a torque acts. A net force appears only in a non-uniform field, which is why PE changes and the dipole drifts toward stronger field.

Is U = -pE cosθ valid in a non-uniform field?

Strictly, U = -pE cosθ is derived for a uniform field. In a non-uniform field the field varies over the dipole, so a net force also appears, but for NEET the principle 'the dipole moves to lower U = -p·E' still guides the answer.