318 ELECTRICAL APPARATUS mediate speeds, which are only approximated by the transformer theory of the single-phase induction motor. For studying the action of the motor at intermediate and at low speed, as for instance, when investigating the performance of a starting device, in bringing the motor up to speed, that is, during acceleration, this method so is more suited. An applica- tion to the "condenser motor/' that is, a single-phase induction motor using a condenser in a stationary tertiary circuit (under an angle, usually 60°, with the primary circuit) is given in the paper on "Alternating-Current Motors," A. I. E. E. Transac- tions, 1904. P&D 120 110 100 90 80 70 60 50 40 30 20 10 ^+*~ . -------- — --^ — — — . ""^•^ i ^"' s"*xs -650 "^ \ -600 SINGLE PHASE INDUCTION MOTOR 400 VOLTS j>^- ^N —550 / > \ \ —500 ^x X^XN v —450 / * / V xsx —400 • /" / x XX^ A « 350 . °x /"' ^^ X Ml ,*>f)A ........ ^ Xp^. .^--"" "/ x^ \\ -250-- onn — - ^" ~'~ p/. ^ ^ V J ,. __ . — —*•—"""" /" X i^r \\ i - -IKft- ......... " /\ ^ ^. *^ ¥T ^ X ^< ^ ^ ~" L^== o :£^- ^- — ' I .2 .3 .4 .5 .6 .7 .8 .9 100 so 70 60 50 40 30 20 10 TIG. 151. 180. As example are shown, in Fig. 151, with the speed as abscissae, the curves of a single-phase induction motor, having the constants: e0 = 400 volts, 1 = 1 + 10 j ohms, and: hence: ZQ = Zi = 0.1 + 0.3 j ohms; N lo = 400 ••:=: amp. ; N = (s0 + 0.2) + j(10so + 0.6 - 0.6S)-, ' K = (0.1 + 0.3 j) N+ (1 + 10 j)(0.1 + j) (0.3-0. JD synchronous kw.