D. C. COMMUTATING MACHINES 187 ampere-turns per pole. Choosing then 8000 ampere-turns per commutating pole F', leaves 2000 ampere-turns as resultant com- mutating m.m.f . at full load, half as much at half load, etc. The resultant m.m.f. of the main field FQ, the armature Fa, and the commutating pole Ff is represented in Fig. 100 by Fz, and the flux produced by it is shown in Fig. 101. As seen, with the com- mutator brushes midway between the field poles, that is, in the center of the commutating pole, a commutating flux proportional to the armature current enters the armature at the brush B and 5', and is cut by the revolving armature during commutation. The use of the commutating pole or interpole thus permits controlling the commutation, with fixed brush position midway between the field poles, and commutating poles therefore are FIG. 101. — Magnetic flux distribution with commutating pole. extensively used in larger machines, especially of the high-speed type. The commutating pole makes the commutation independent of the main field strength, and therefore permits the machines to operate with equally good commutation over a wide voltage range, and at low voltage, that is, low field strength, as required for instance in boosters, etc. 50. With multiple-wound armatures, at least one commutat- ing pole for every pair of main poles is required, while with a series-wound armature a single commutating pole would be sufficient for all the sets of armature brushes, if of sufficient strength. In general, however, as many commutating poles as main poles are used. With the position of the brushes at the neutral, as is the case when using commutating poles, the armature reaction has no 188 ELEMENTS OF ELECTRICAL ENGINEERING demagnetizing component, and the only drop of voltage at load is that due to the armature resistance drop and the distortion of the main field, which at saturation produces a decrease of the total flux, as shown in Fig. 98. As is seen in Fig. 101, the magnetic flux of the commutating pole is not symmetrical, but the spread of flux is greater at the side of the main pole of the same polarity. As result thereof, the total magnetic flux is slightly increased by the commutating poles; that is, the two halves of the commutating flux on the two sides of the brush do not quite neutralize, and the com- mutating flux thus exerts a slight compounding action, that is, tends to raise the voltage. This can be still further increased by shifting the brushes slightly back and thus giving a magnet- izing component of armature reaction. This can be done with- out affecting commutation as long as the brushes still remain under the commutating pole. In this manner a compounding or even a slight over-compounding can be produced without a series winding on the main field poles, or, inversely, by shifting the brushes slightly forward, a demagnetizing component of armature reaction can be introduced. Furthermore, the current induced in the short-circuited armature coil by the commutating field is magnetizing, that induced by the magnetic field of arma- ture reaction, demagnetizing. In operating machines with commutating poles in multiple, care therefore must be taken not to have the compounding action of the commutating poles interfere with the distribution of load ; for this purpose an equalizer connection may be used between the commutating pole windings of the different machines, and the commutating windings treated in the same way as series coils on the main poles, that is, equalized between the different machines to insure division of load. 51. The advantage of the commutating pole over the shift of brushes to the edge of the next field pole, in constant poten- tial machines — shunt or compound wound — thus is that the commutating flux of the former has the right intensity at all loads, while that of the latter is right only at one particular load, too high below, too low above that load. In series-wound machines, that is, machines in which the main field is excited in series with the armature, and thus varies in strength with the armature current, armature reaction and field excitation are Always proportional to each other, and the distribution of mag-