The net force on a current-carrying coil in a uniform magnetic field is zero because the magnetic field exerts equal and opposite forces on opposite sides of the coil.
However, the coil experiences a torque \( \tau \), which tends to align the coil’s magnetic dipole moment \( \mathbf{M} \) with the external magnetic field \( \mathbf{B} \). The torque is given by:
\[
\tau = \mathbf{M} \times \mathbf{B}
\]
The coil will be in stable equilibrium when \( \mathbf{M} \) is aligned with \( \mathbf{B} \). In this orientation, the potential energy of the coil is minimized, and the flux of the total magnetic field through the coil is maximum.
The total flux \( \Phi_{\text{total}} \) through the coil is:
\[
\Phi_{\text{total}} = B A \cos(\theta)
\]
Where \( \theta \) is the angle between the magnetic field and the normal to the coil’s surface.
At stable equilibrium, \( \theta = 0 \), and the flux is maximized.