A current-carrying coil within a uniform magnetic field experiences zero net force. This is due to the magnetic field applying equal and opposing forces on opposite sides of the coil. However, a torque \( \tau \) is generated, aiming to align the coil’s magnetic dipole moment \( \mathbf{M} \) with the external magnetic field \( \mathbf{B} \). The torque is mathematically expressed as:\[\tau = \mathbf{M} \times \mathbf{B}\]Stable equilibrium is achieved when \( \mathbf{M} \) is parallel to \( \mathbf{B} \). In this configuration, the coil's potential energy is at its minimum, and the total magnetic field flux through the coil is maximized.The total flux \( \Phi_{\text{total}} \) through the coil is calculated as:\[\Phi_{\text{total}} = B A \cos(\theta)\]Here, \( \theta \) represents the angle between the magnetic field and the normal vector of the coil’s surface.When \( \theta = 0 \), the coil is in stable equilibrium, and the flux is at its maximum value.