As a motor’s armature rotates, its conductors cut through the magnetic field, inducing a voltage according to Faraday’s law of induction. This ‘back-EMF’ opposes the main voltage driving the motor. Its magnitude is directly proportional to the motor’s rotational speed (\(\mathcal{E}_{back} \propto \omega\)). This phenomenon is crucial for the self-regulation of motor speed and current draw.











