Question:

A magnetic dipole experiences a torque of \( 80\sqrt{3} \) N m when placed in a uniform magnetic field in such a way that the dipole moment makes an angle of \( 60^\circ \) with the magnetic field. The potential energy of the dipole is:

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Remember the formulas for the torque \( \tau = MB \sin \theta \) and potential energy \( U = -MB \cos \theta \) of a magnetic dipole in a uniform magnetic field. Use the given torque and angle to find the product \( MB \), and then use this value to calculate the potential energy at the same angle.
Updated On: Apr 25, 2025
  • 80 J
  • \( -40\sqrt{3} \) J
  • -60 J
  • -80 J
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The Correct Option is D

Solution and Explanation

The torque \( \tau \) experienced by a magnetic dipole in a uniform magnetic field \( \vec{B} \) is given by: \[ \tau = \vec{M} \times \vec{B} = MB \sin \theta \] where \( M \) is the magnitude of the magnetic dipole moment, \( B \) is the magnitude of the magnetic field, and \( \theta \) is the angle between \( \vec{M} \) and \( \vec{B} \). Given \( \tau = 80\sqrt{3} \) N m and \( \theta = 60^\circ \). \[ 80\sqrt{3} = MB \sin 60^\circ \] \[ 80\sqrt{3} = MB \left( \frac{\sqrt{3}}{2} \right) \] \[ MB = \frac{80\sqrt{3} \times 2}{\sqrt{3}} = 160 \] The potential energy \( U \) of the magnetic dipole in the uniform magnetic field is given by: \[ U = -\vec{M} \cdot \vec{B} = -MB \cos \theta \] Substituting the values \( MB = 160 \) and \( \theta = 60^\circ \): \[ U = -(160) \cos 60^\circ \] \[ U = -160 \left( \frac{1}{2} \right) \] \[ U = -80 \text{ J} \]
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