The simplest commutator is a \split ring" that makes contact with two separate brushes. In the simple AC loop generator, the rotating and xed conductors are connected with two slip rings, each of which maintains a continuous connection between one end of the rotating loop and a xed wire. The split ring commutators joins both ends of the loop to xed wires, and every half-rotation, the contacts are switched. In a generator, the simple split ring commutator on a single loop gener-ator would produce a voltage (and current) around the loop that is a single rectied sine wave, varying between zero and maximum every quarter rev-solution. In a DC motor with a simple split ring commutator, the torque provide by the motor is similarly irregular, varying from zero to maximum every quarter revolution. The motor doesn't provide steady even rotational force but a jerky force, wich is obviously not ideal for industrial applications. This is termed \torque ripple." To minimize torque ripple, DC motors use the same strategies that DC generators use to minimize voltage ripple: in-creasing the number of windings on the rotor or magnetic poles on the stator. (The windings on the rotor are also called the \armature"). By producing many out-of-sync rectied sine waves superimposed on each other, adding windings or poles begins to approximate a constant torque.
Brushed DC motors seem like a relatively practical solution, but there are drawbacks. The brushes themselves wear out fairly fast, and it is not wise to put big amounts of current through brushes that make sliding contacts, as they will spark as contacts are made and then broken. If the rotor turns too quickly, the sparking can damage or destroy the commutator. Designing a brushed DC motor involves tradeoffs between power, speed, and repair frequency/cost.
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