354 ELECTRICAL APPARATUS consumed by it is wattless and therefore produces no serious heating and reactive leads of low resistance thus are not liable to self-destruction by heating if the motor fails to start im- mediately. On account of the limited space available in the railway motor considerable difficulty, however, is found in designing sufficiently high reactances which do not saturate and thus decrease at larger currents. At speed, reactance in the armature coils is very objectionable in retarding the reversal of current, and indeed one of the most important problems in the design of commutating machines is to give the armature coils the lowest possible reactance. There- fore, the insertion of reactance in the motor leads interferes seriously with the commutation of the motor at speed, and thus requires the use of a suitable commutating or reversing flux, that is, a magnetic field at the commutator brushes of sufficient strength to reverse the current, against the self-inductance of the armature coil, by means of an e.m.f. generated in the armature coil by its rotation. This commutating flux thus must be in phase with the main current, that is, a flux of overcompensation. Reactive leads require the use of a commutating flux of over- compensation to give fair commutation at speed. Counter E.m.fs. in Commutated Coil 199. Theoretically, the correct way of eliminating the de- structive effect of the short-circuit current under the commu- tator brush resulting from the e.m.f. of alternation of the main flux would be to neutralize the e.m.f. of alternation by an equal but opposite e.m.f. inserted into the armature coil or generated therein. Practically, however, at least with most motor types, considerable difficulty is met in producing such a neutralizing e.m.f. of the proper intensity as well as phase. Since the alter- nating current has not only an intensity but also a phase displace- ment, with an alternating-current motor the production of corn- mutating flux or commutating voltage is more difficult than with direct-current motors in which the intensity is the only variable. By introducing an external e.m.f. into the short-circuited coil under the brush it is not possible entirely to neutralize its e.m.f. of alternation, but simply to reduce it to one-half. Several such arrangements were developed in the early days by Eickemeyerj