Given:
The potential energy \( U \) of a magnetic dipole in a uniform magnetic field is given by the formula:
\[ U = -MB \cos \theta \]
Since the magnetic moment is initially aligned with the magnetic field, \( \theta = 0^\circ \), and thus:
\[ U = -MB \cos(0^\circ) = -MB \]
Substitute the values:
\[ U = -5 \times 0.4 = -2 \, \text{J} \]
Thus, the potential energy of the bar magnet is -2 J.
When the magnet is turned by 180°, the angle between the magnetic moment and the magnetic field becomes \( \theta = 180^\circ \). The new potential energy is:
\[ U' = -MB \cos(180^\circ) = +MB \]
Substitute the values:
\[ U' = +5 \times 0.4 = +2 \, \text{J} \]
The work done in turning the magnet is the change in potential energy:
\[ W = U' - U = 2 - (-2) = 4 \, \text{J} \]
Thus, the work done in turning the magnet by 180° is 4 J.
A short bar magnet placed with its axis at 30º with a uniform external magnetic field of 0.25 T experiences a torque of magnitude equal to 4.5 × 10-2 J. What is the magnitude of magnetic moment of the magnet?
A short bar magnet of magnetic moment m = 0.32 J T-1 is placed in a uniform magnetic field of 0.15 T. If the bar is free to rotate in the plane of the field, which orientation would correspond to its ( a ) stable, and ( b) unstable equilibrium? What is the potential energy of the magnet in each case?
A closely wound solenoid of 800 turns and area of cross section 2.5 × 10-4 m2 carries a current of 3.0 A. Explain the sense in which the solenoid acts like a bar magnet. What is its associated magnetic moment?