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.
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Start your 14-day free trial to unlock the full solution →Part 1: torque on a bar magnet = (pole strength × B) × (perpendicular separation between the two forces) = . Part 2 (OR): a solenoid's interior field from Ampere's law is .
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, (north) and (south), separated by the magnetic length . Its magnetic dipole moment is
a vector of magnitude , directed from the south pole to the north pole, SI unit A·m².
Torque derivation: Place the bar magnet in a uniform magnetic field , with its axis making angle with . Each pole experiences a force of magnitude :
- On the N-pole: force along .
- On the S-pole: force opposite to .
These two equal, opposite, parallel (but not collinear) forces form a couple. The perpendicular distance between their lines of action is (the component of the pole separation perpendicular to ).
Torque = one force × perpendicular distance between the forces:
In vector form: . This torque tends to rotate/align the magnet's dipole moment along ; it is zero when (, stable equilibrium) and maximum when .
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 ():
Consider a long solenoid with turns per unit length carrying current . 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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