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Torque on a Magnetic Dipole (Bar Magnet) in a Uniform Magnetic Field

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Estimated time: 5 minutes
CISCE: Class 12

Introduction

A freely suspended bar magnet rotates when placed in a uniform magnetic field and finally comes to rest with its magnetic moment aligned along the field.

This turning effect is called torque.

Core idea: A magnetic field exerts a torque on a magnetic dipole, tending to align its magnetic dipole moment \[\vec m\] with the magnetic field \[\vec B\].

CISCE: Class 12

Derivation of Torque

Consider a bar magnet as N aligned current loops, each of area A, carrying current I.

For one current loop in a uniform magnetic field: τone loop = I A B sin⁡ θ

For N identical aligned loops:

τ = N (IAB sin⁡ θ)
τ = (NIA) B sin⁡ θ

For a magnetic dipole, m = NIA

Therefore, τ = m B sin⁡ θ

Vector form: \[\vec τ\] = \[\vec m\] × \[\vec B\]

Important: θ is always measured between \[\vec m\] and \[\vec B\].

CISCE: Class 12

Special Cases and Equilibrium

Orientation of \[\vec m\] relative to \[\vec m\] θ Torque Nature of position
Parallel 0 Stable equilibrium
Perpendicular 90° Maximum: τmax = mB Maximum turning effect
Antiparallel 180° 0 Unstable equilibrium

Maximum torque

  • When θ = 90°, τmax ⁡= mB
  • Hence, m = \[\frac {τ_{max}}{⁡B}\]

Zero torque: τ = 0 when θ = 0° or 180°

SI Unit of Magnetic Dipole Moment:

m = \[\frac {τ}{B}\]​ = \[\frac {N m}{T}\]

Since 1 T = 1 N A−1m−1

[m] = A m2

Shaalaa.com | Matter and Magnetism part 6 (Dipole in Uniform Magnetic field -1)

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Matter and Magnetism part 6 (Dipole in Uniform Magnetic field -1) [00:11:10]
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