382 ELECTRICAL APPARATUS where nr with a fractional-pitch armature winding is the number of series turns in the pitch angle, o>, that is: nr = — nf IT n" being the number of turns in series between the brushes, since in the space (TT — «) outside of the pitch angle the armature conductors neutralize each other, that is, conductors carrying current in opposite direction are superposed upon each other. See fractional-pitch windings, chapter "Commutating Machine," " Theoretical Elements of Electrical Engineering/' 212. Let: Eo, Jo, ZQ = impressed voltage, current and self-inductive impedance of the magnetizing or exciter circuit of stator (field coils), reduced to the rotor energy circuit by the ratio of effective turns, Co, Eiy Ji, Zi = impressed voltage, current and self-inductive im- pedance of the rotor energy circuit (or circuit at right angles to Jo), Ez, J2, £2 = impressed voltage, current and self-inductive im- pedance of the stator compensating circuit (or circuit parallel to Ji) reduced to the rotor circuit by the ratio of effective turns, c2. E3, h, Zi = impressed voltage, current and self-inductive im- pedance of the exciting circuit of the rotor, or circuit parallel tO IQj J4, Z4 = current and self -inductive. impedance of the short- circuit under the brushes, Ji, reduced to the rotor circuit, J5, Z5 = current and self-inductive impedance of the short- circuit under the brushes, J3, reduced to the rotor circuit, Z = mutual impedance of field excitation, that is, in the direc- tion Of Jo, 13, I*, Zr = mutual impedance of armature reaction, that is, in the direction of Ji, J2, Js- Zr usually either equals Z, or is smaller than Z. 14 and JB are very small, Z& and Z5 very large quantities. Let S = speed, as fraction of synchronism. Using then the general equations 7 Chapter XIX, which apply to any alternating-current circuit revolving with speed, S, through a magnetic field energized by alternating-current circuits, gives for the six circuits of the general single-phase commutator motor the six equations: