Table of Contents

Graph

le torque is applied to le coil

Why does this work? Right hand rule

IF we just keep this position, the motor will rotate back and forth, i.e. not uni-directionally. This occurs because at some point in the revolution, the direction of torque will flip. So we use a commutator to switch the currents so this doesn't happen!

This makes a torque!

Force on one wire on one side: $F=IlB$ Force per coil, given $N$ turns of a coil: $F=NIlB$ Hence, as $\tau=rF\sin \theta$, $\tau = rNIlB\sin \theta$ - One side!!!

Hence, if we consider the other side: $\tau_{\text{max}}=2NIlBr\sin \theta$

This is the maximum torque on a coil in a motor.

But consider that $2lr$ is essentially $ld$ where d is the diameter. Hence, we can represent this as $A$, i.e. the area of the shape of the coil.

Hence, $\tau_{\text{max}}=NIAB\sin \theta$

Note that torque will change over time.