1. Magnetic Potential Energy: The magnetic potential energy (U) of a magnetic dipole (magnetic moment $\vec{m}$) in a magnetic field $\vec{B}$ is given by:
\[ U = -\vec{m} \cdot \vec{B} = -mB \cos\theta \]
where $\theta$ is the angle between the magnetic moment vector and the magnetic field vector.
2. Perpendicular Orientation ($\theta = 90^\circ$): When the magnetic bar is placed perpendicular to the magnetic field, the angle $\theta$ is $90^\circ$. Therefore, $\cos\theta = \cos(90^\circ) = 0$.
\[ U = -mB(0) = 0 \]
3. Conclusion: The magnetic potential energy is zero when the magnetic moment is perpendicular to the magnetic field.
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is: