D. C. COMMUTATING MACHINES 183 In Figs. 96, 97, 98, 99, curves are plotted corresponding to those in Figs. 92, 93, 94, and 95. As seen, the spread of mag- netic flux at the pole corners is greatly increased, but farther away from the field poles the magnetic distribution is not changed. 47. The magnetizing, or rather demagnetizing, effect of the load with shifted brushes is not changed. The distorting effect FIG. 96. — Flux distribution under a single pole. of the load is, however, very greatly decreased, to a small per- centage of its previous value, and the magnetic field under the field pole is very nearly uniform under load. The reason is: Even a very large increase of m.m.f. does not much increase the density, the ampere-turns being consumed by saturation of the iron, and even with a large decrease of m.m.f. the density is not decreased much, since with a small decrease 'I/ • \\ L FIG. 97. — Distribution of flux and m.m.f. at no load. of density the ampere-turns consumed by the saturation of the iron become available for the air gap. Thus, while in Fig. 95 the densities at the center and the two pole corners of the field pole are 8000, 12,000, and 4000, with the saturated structure in Fig. 99 they are 8000, 9040, and 6550. At or near the theoretical neutral, however, the saturation has no effect. That is, saturation of the armature teeth affords a means of 184 ELEMENTS OF ELECTRICAL ENGINEERING reducing the distortion of the magnetic field, or the shifting of flux at the pole corners, and is thus advantageous for machines which shall operate over a wide range of load with fixed position of brushes, if the brushes are shifted near to the next following pole corner. Fo J FIG. 98. — Distribution of flux and m.m.f. at load, with Brushes at neutral. It offers no direct advantage, however, for machines corn- mutating with the brushes midway between the field poles, as converters. An effect similar to saturation in the armature teeth is produced J L FIG. 99. — Distribution of flux and m.m.f. at load, with brushes shifted to next pole corner. by saturation of the field pole face, or more particularly, satura- tion of the pole corners of the field.