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Q.What is magnetic dipole moment? Derive the expression for torque on a bar magnet placed in a uniform magnetic field. OR What is a solenoid? Derive the expression for magnetic field due to a long current carrying solenoid by using Ampere's circuital law.

Manipur CohsemCOHSEM Manipur Higher Secondary Board 2018Subjective· 5mImportance★★★★★
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Part 1: torque on a bar magnet = (pole strength × B) × (perpendicular separation between the two forces) = mBsin⁡θmB\sin\theta. Part 2 (OR): a solenoid's interior field from Ampere's law is B=μ0nIB=\mu_0 nI.

Part 1 — Magnetic dipole moment and torque on a bar magnet

A bar magnet behaves as a magnetic dipole: two equal and opposite magnetic poles, +qm+q_m (north) and −qm-q_m (south), separated by the magnetic length 2l2l. Its magnetic dipole moment is

m⃗=qm(2l⃗)\vec m = q_m(2\vec l)

a vector of magnitude m=qm×2lm=q_m\times 2l, directed from the south pole to the north pole, SI unit A·m².

Torque derivation: Place the bar magnet in a uniform magnetic field B⃗\vec B, with its axis making angle θ\theta with B⃗\vec B. Each pole experiences a force of magnitude F=qmBF = q_mB:

  • On the N-pole: force qmBq_mB along B⃗\vec B.
  • On the S-pole: force qmBq_mB opposite to B⃗\vec B.

These two equal, opposite, parallel (but not collinear) forces form a couple. The perpendicular distance between their lines of action is 2lsin⁡θ2l\sin\theta (the component of the pole separation perpendicular to B⃗\vec B).

Torque = one force × perpendicular distance between the forces:

τ=F×(2lsin⁡θ)=qmB×2lsin⁡θ=(qm⋅2l)Bsin⁡θ=mBsin⁡θ\tau = F\times(2l\sin\theta) = q_mB\times 2l\sin\theta = (q_m\cdot 2l)B\sin\theta = mB\sin\theta

In vector form: τ⃗=m⃗×B⃗\vec\tau = \vec m\times\vec B. This torque tends to rotate/align the magnet's dipole moment m⃗\vec m along B⃗\vec B; it is zero when m⃗∥B⃗\vec m \parallel \vec B (θ=0\theta=0, stable equilibrium) and maximum when θ=90°\theta=90°.


Part 2 (OR) — Magnetic field of a long current-carrying solenoid

A solenoid is a long, tightly-wound helical coil of wire; when carrying current, it produces a magnetic field very similar to that of a bar magnet, with a strong, nearly uniform field inside and a weak field outside.

Derivation using Ampere's circuital law (∮B⃗⋅dl⃗=μ0Ienc\oint \vec B\cdot d\vec l = \mu_0 I_{enc}):

Consider a long solenoid with nn turns per unit length carrying current II. For an ideal long solenoid, the field outside is taken as negligible, and the field inside is uniform and parallel to the axis.

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