Force and Torque on a Current Loop
A current loop in a uniform magnetic field feels no net force (the forces on opposite sides cancel) but it does feel a torque, and that torque is what turns every electric motor. The loop behaves like a little bar magnet with magnetic moment $\mathbf{m} = N I A\,\hat{\mathbf{n}}$, and the field twists it with $\boldsymbol{\tau} = \mathbf{m}\times\mathbf{B}$, of size $N I A B\sin\theta$, largest when the loop faces along the field and zero when its moment is aligned with $\mathbf{B}$. Left free, the loop swings like a pendulum and settles with $\mathbf{m}$ parallel to $\mathbf{B}$. Add a commutator that flips the current every half turn, right where the torque would otherwise reverse, and the loop spins continuously: that is a direct-current motor, and the lumpy $|\sin\theta|$ torque is the torque ripple real motors smooth out with many windings.
WHAT TO TRY
- Watch the free loop swing and settle with its moment $\mathbf{m}$ (purple) aligned along $\mathbf{B}$; that is the stable zero of the torque curve.
- Note the force couple (red) is largest when the loop faces the field (torque maximal) and does no turning when $\mathbf{m}$ points along $\mathbf{B}$ (torque zero).
- Toggle to motor: the commutator flips the current each half turn, the current and forces reverse, and the loop spins one way continuously.
- Raise the load and the motor settles to a lower terminal speed; raise the field or current and it spins faster, as the dashed terminal line shows.