Q.An electric dipole with dipole moment 4×10−9C m is aligned at 30∘ with the direction of a uniform electric field of magnitude 5×104N C−1. Calculate the magnitude of the torque acting on the dipole.
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Torque on a Dipole — From Intuition to the Formula
Imagine a bar magnet placed in a uniform magnetic field. You know that the north pole gets pulled one way and the south pole the opposite way. If the magnet is not aligned with the field, these two equal and opposite forces create a twist — a torque — that tries to rotate the magnet until it lines up with the field. That's the core idea.
The same thing happens with an electric dipole (two equal and opposite charges +q and −q separated by a small distance d) placed in a uniform electric field E. The two charges experience forces in opposite directions, and unless the dipole is already parallel to the field, those forces produce a torque.
Step 1: The Forces on the Two Charges
Let the dipole moment p point from the negative charge to the positive charge, with magnitude p=qd.
In a uniform electric field E:
- The positive charge +q feels a force F+=+qE (in the direction of E).
- The negative charge −q feels a force F−=−qE (opposite to E).
These two forces are equal in magnitude but opposite in direction. They form a couple — a pair of equal, opposite, parallel forces that do not share the same line of action. A couple always produces a pure torque, with no net force.
Step 2: Why a Torque Appears
If the dipole is at an angle θ to the field, the two forces are not along the same line. They are separated by the perpendicular distance between their lines of action. That perpendicular distance is dsinθ, where d is the separation between the charges.
The torque τ due to a couple is:
τ=(force magnitude)×(perpendicular distance between forces)
Here:
- Force magnitude on each charge: F=qE
- Perpendicular distance: dsinθ
So:
τ=(qE)×(dsinθ)=qdEsinθ
But qd=p, the magnitude of the dipole moment. Therefore:
τ=pEsinθ
Step 3: The Vector Form
Torque is a vector — it has a direction. The direction of the torque is perpendicular to both p and E, following the right-hand rule. The complete vector equation is:
τ=p×E
The magnitude is ∣τ∣=pEsinθ, where θ is the angle between p and E.
Step 4: What the Torque Does
- When θ=0∘ (dipole aligned with the field): sin0=0, so τ=0. The dipole is in stable equilibrium — if you nudge it slightly, the torque brings it back.
- When θ=90∘ (dipole perpendicular to the field): sin90∘=1, so torque is maximum: τmax=pE. …
Why this formula?
Torque on a Dipole in a Uniform Electric Field
Let's build this from first principles — understanding why the torque formula is what it is, not just memorizing it.
What is a Dipole?
A dipole consists of two equal and opposite charges +q and −q, separated by a small distance 2a (or d). The dipole moment vector is:
p=q⋅d
where d points from −q to +q, and ∣d∣=2a.
The Physical Situation
Place this dipole in a uniform external electric field E. Uniform means the field has the same magnitude and direction everywhere.
- The +q charge experiences a force: F+=+qE
- The −q charge experiences a force: F−=−qE
These two forces are equal in magnitude but opposite in direction.
Why is there a Torque?
Since the forces are equal and opposite, the net force on the dipole is zero:
Fnet=qE+(−qE)=0
So the dipole won't accelerate linearly. But — crucially — the two forces act at different points in space (the two charges are separated). This creates a couple (a pair of equal, opposite, parallel forces not acting along the same line). A couple always produces a torque (rotational effect).
Deriving the Torque Magnitude
Let the dipole be oriented at an angle θ with respect to the field E.
- The line joining the charges makes angle θ with E.
- The perpendicular distance between the lines of action of the two forces is the "lever arm."
Step 1: The force on each charge is qE.
Step 2: The perpendicular distance between the two forces is:
Lever arm=2asinθ
Why sinθ? Because the separation vector d is at angle θ to E. The component of d perpendicular to E is dsinθ=2asinθ.
Step 3: Torque = Force × Perpendicular distance (for one force about the midpoint):
τ=(qE)×(2asinθ)
Step 4: But q×2a=p, the dipole moment magnitude. So:
τ=pEsinθ
Vector Form — The Full Picture
Torque is a vector. Its direction is given by the right-hand rule: it tends to rotate the dipole toward alignment with the field.
The vector form captures both magnitude and direction:
τ=p×E
- Magnitude: ∣τ∣=pEsinθ (as derived)
- Direction: Perpendicular to both p and E, given by the cross product rule.
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Concept: Torque on an Electric Dipole
When an electric dipole of moment p is placed in a uniform electric field E, it experiences a torque that tries to align it with the field. The magnitude of this torque is given by
τ=pEsinθ
where θ is the angle between the dipole moment and the electric field direction.
Calculation:
Given:
- Dipole moment: p=4×10−9C m
- Electric field: E=5×104N C−1
- Angle: θ=30∘
Substituting into the torque formula: …
A dipole in a uniform field experiences maximum torque when perpendicular to the field and zero when aligned; here at 30° the torque is τ=pEsinθ=10−4N m.
Why a dipole experiences torque
An electric dipole consists of two equal and opposite charges separated by a small distance. When placed in a uniform electric field, both charges experience forces of equal magnitude but in opposite directions. Because the charges are spatially separated, these forces don't simply cancel—they create a couple that tries to rotate the dipole.
The key insight is that the torque depends on how misaligned the dipole is with the field. When the dipole moment vector p points along the field E, the forces on both charges lie along the dipole axis and produce no rotation. When perpendicular, the lever arm is maximum and torque peaks. At any intermediate angle θ, only the component of force perpendicular to the dipole axis contributes to rotation.
τ=pEsinθ
where p is the dipole moment magnitude, E is the field strength, and θ is the angle between p and E.
Step-by-step calculation
-
Identify the given quantities
- Dipole moment: p=4×10−9C m
- Electric field: E=5×104N C−1
- Angle between dipole and field: θ=30°
-
Recognize the torque formula
The magnitude of torque on a dipole in a uniform field is the cross-product magnitude:
τ=∣p×E∣=pEsinθ …
Instead of applying τ=pEsinθ directly, derive the torque from the dipole's potential energy in the field — torque is the rate of change of energy with orientation. Both routes give τ=1×10−4N m.
Method: Torque from the Potential Energy Function
A dipole in a uniform field doesn't just feel a torque — it has an orientation-dependent potential energy. Torque is nothing but how fast that energy changes as you rotate the dipole, which gives an equivalent, more general way to arrive at the same result.
- Write down the potential energy of the dipole. When a dipole moment p makes angle θ with a uniform field E, its potential energy is
U(θ)=−pEcosθ
This is lowest (most stable) when p is aligned with E (θ=0) and highest when anti-aligned (θ=180°) — exactly what we'd expect physically.
- Recall the rotational analogue of F=−dxdU. For rotation, the torque about an axis is the negative derivative of potential energy with respect to the rotation angle:
τ=−dθdU
- Differentiate. τ=−dθd(−pEcosθ)=pEsinθ …
Step 1 — The Correct Formula
The torque τ on an electric dipole in a uniform electric field E is:
τ=p×E
Magnitude:
τ=pEsinθ
Where:
- p = dipole moment magnitude
- E = electric field magnitude
- θ = angle between p and E
Step 2 — Apply the Given Data
Given:
- p=4×10−9C m
- E=5×104N C−1
- θ=30∘
So:
τ=(4×10−9)×(5×104)×sin30∘
τ=20×10−5×21
τ=10×10−5=1.0×10−4N m
Answer: 1.0×10−4N m
Common Mistakes Students Make
✗ Mistake 1: Using cosθ instead of sinθ
- Why it happens: Students confuse torque with the formula for potential energy (U=−pEcosθ).
- How to avoid:
- Torque comes from the cross product → use sinθ.
- Potential energy comes from the dot product → use cosθ.
- Remember: Torque is maximum when dipole is perpendicular (θ=90∘) — that’s sin90∘=1, not cos90∘=0.
✗ Mistake 2: Taking θ as the angle with the field direction incorrectly
- Why it happens: Some problems give the angle between dipole and field as 60∘ or 120∘, and students use that directly without checking.
- How to avoid:
- θ in τ=pEsinθ is always the angle between p and E.
- If the problem says “aligned at 30∘ with the field”, that’s exactly θ=30∘ — correct here.
✗ Mistake 3: Forgetting to convert units or misreading powers of 10
- Why it happens: p is given in 10−9 and E in 104 — students sometimes multiply without tracking exponents.
- How to avoid:
- Write all numbers in scientific notation before multiplying.
- Do exponent arithmetic separately: 10−9×104=10−5.
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- GSEB Higher Secondary Certificate (HSC) Examination 2026Set ANNUAL1 markMCQQ.An electric dipole with dipole moment 4 x 10^-9 C m is aligned at 30 degrees with the direction of a uniform electric field of magnitude 5 x 10^4 NC^-1. What is the magnitude of the torque acting on the dipole?(a) 10^-4 Nm(b) 10^4 Nm(c) 10^2 Nm(d) 10^-2 Nm
›Reveal solutionSolution
The torque on an electric dipole in a uniform external field is tau = p E sin(theta), where theta is the angle between the dipole moment and the field.
Given p = 4 x 10^-9 C m, E = 5 x 10^4 N/C, theta = 30 degrees, sin(30) = 0.5.
…
- GUJCET 2024Set 131 markMCQQ.For an electric dipole an angle between E and P at a point on the equatorial plane is ________. (A) 45∘ (B) 180∘ (C) 0∘ (D) 90∘
›Reveal solutionSolution
On the equatorial (perpendicular-bisector) plane of a dipole, the field E is directed antiparallel to the dipole moment P, giving an angle of 180∘. …
- GUJCET 2024Set 131 markMCQQ.A short bar magnet placed with its axis at 30∘ with a uniform external magnetic field of 0.5 T experiences a torque of magnitude equal to 4.5×10−2 J. Then the magnitude of magnetic moment of the magnet will be ________. (A) 18×10−2 JT−1 (B) 36×10−2 JT−1 (C) 1.8×102 JT−1 (D) 3.6×102 JT−1
›Reveal solutionSolution
Torque on a magnet τ=mBsinθ; solve for m.
Concept. A magnetic dipole in a field feels torque τ=mBsinθ. …
- GUJCET 2022Set 171 markMCQQ.A short bar magnet placed with its axis at 30° with a uniform external magnetic field of 0.25 T experiences a torque of magnitude equal to 4.5×10−2 J. What is the magnitude of magnetic moment of the magnet? (A) 0.36 J T−1 (B) 0.036 J T−1 (C) 3.6 J T−1 (D) 36 J T−1
›Reveal solutionSolution
From τ=mBsinθ: m=Bsinθτ=0.36 J T⁻¹.
Concept: τ=mBsinθ, so …
- GUJCET 2020Set 071 markMCQQ.A coil having 10Am2 magnetic moment is placed in a vertical plane & is free to rotate about its horizontal axis coincides with its diameter. A uniform magnetic field of 2T in the horizontal direction exists such that initially the axis of the coil is in the direction of the field. The coil rotates through an angle of 90∘ under the influence of magnetic field. The moment of Inertia of coil is 0.1kgm2. What will be its angular speed? (A) 20 rad/s (B) 10 rad/s (C) 5 rad/s (D) 40 rad/s
›Reveal solutionSolution
The magnetic PE released, mB(cos0−cos90∘)=mB=20J, becomes 21Iω2, giving ω=20 rad/s.
Concept — magnetic dipole in a field, energy method. A magnetic dipole has U(θ)=−m⋅B=−mBcosθ. Initially the coil's diameter axis lies along B, so the moment (normal to the coil plane) is perpendicular to B (θ=90∘, U=0). It rotates 90∘ so the moment aligns with B (θ=0, U=−mB), releasing energy. …
- GUJCET 2019Set 131 markMCQQ.An electric dipole is placed in a nonuniform electric field, then............. (A) Torque acting on it is always zero (B) The resultant force acting on the dipole may be zero (C) Torque acting on it may be zero (D) The resultant force acting on the dipole is always zero
›Reveal solutionSolution
[!TLDR]
In a non-uniform field the resultant force is generally non-zero, while the torque can be zero when p∥E.
Concept
Torque on a dipole is τ=p×E, which vanishes when the dipole moment is parallel or antiparallel to the field. In a non-uniform field the two charges of the dipole experience unequal forces, so there is generally a non-zero net force as well (unlike a uniform field, where the net force is always zero).
Solution
- (A) 'Torque always zero' - false; torque is generally non-zero. …
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.What will be the magnitude of torque on an electric dipole having dipole moment of 4 x 10^-9 cm placed in a uniform electric field of intensity of 5 x 10^4 NC^-1 making an angle 180 degree with the field.(a) 10^-4 N-m(b) 0 (zero)(c) 2 x 10^-4 N-m(d) 10^-6 N-m
›Reveal solutionSolution
Torque on a dipole is tau = pE sin(theta); at theta = 180 degree the sine is zero, so the torque is zero.
The torque on an electric dipole in a uniform field is tau = pE sin(theta), where theta is the angle between the dipole moment and the field.
Here theta = 180 degree, so sin(180 degree) = 0.
…
- GUJCET 2014Set A1 markMCQQ.The Earth's magnetic field at some place on magnetic equator of Earth is 0.5×10−4 T. Consider the radius of Earth at that place as 6400 km. Then, magnetic dipole moment of the Earth is __________ Am2 (μ0=4π×10−7 TmA−1) (A) 1.05×1023 (B) 1.31×1023 (C) 1.15×1023 (D) 1.62×1023
›Reveal solutionSolution
[!TLDR] Treating the Earth as a magnetic dipole, its moment is about 1.31×1023 Am2, option (B).
Concept
The magnetic field of a dipole at a point on its equatorial line (the magnetic equator) is B=4πμ0⋅R3m, where R is the distance from the dipole and m the dipole moment. Here μ0/4π=10−7.
Solution
m=μ0/4πBR3=10−7BR3. …
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