Question:

The value of torque \( \boldsymbol{\tau} \) experienced by a current loop of magnetic moment \( \mathbf{m} \) placed in a magnetic field \( \mathbf{B} \) is:

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Torque on magnetic dipole: \[ \boldsymbol{\tau} = \mathbf{m} \times \mathbf{B}. \] Direction is perpendicular to both \( \mathbf{m} \) and \( \mathbf{B} \).
  • \( \boldsymbol{\tau} = \mathbf{m} \times \mathbf{B} \)
  • \( 26 \)
  • \( \boldsymbol{\tau} = \frac{B}{m} \)
  • \( \boldsymbol{\tau} = \mathbf{B} \times \mathbf{m} \)
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The Correct Option is A

Solution and Explanation

The torque \( \boldsymbol{\tau} \) experienced by a magnetic dipole moment \( \mathbf{m} \) placed in a magnetic field \( \mathbf{B} \) is given by the vector cross product: \[ \boldsymbol{\tau} = \mathbf{m} \times \mathbf{B}. \] This torque arises because the magnetic dipole tends to align itself with the external magnetic field. The magnitude of the torque is: \[ |\boldsymbol{\tau}| = m B \sin \theta, \] where \( \theta \) is the angle between the magnetic moment \( \mathbf{m} \) and the magnetic field \( \mathbf{B} \). The direction of the torque is perpendicular to the plane formed by \( \mathbf{m} \) and \( \mathbf{B} \), following the right-hand rule. Physically, this torque causes the magnetic dipole to rotate, reducing the angle \( \theta \) until \( \mathbf{m} \) aligns parallel to \( \mathbf{B} \), minimizing the potential energy of the system.
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