INDUCTION MOTOR 67 45. As further instance, consider the conversion into a, syn- chronous motor of a poor induction motor: a slow-speed motor of very high exciting current, of the constants: e0 = 500; Fo =0.02 - 0.6 j; ZQ = 0.1 + 0.3 j] Zi = 0.1 + 0.3 j. The load curves of this machine as induction motor are given in Pig. 20. LOW SPEED INDUCTION MOTOR DIRECT CURRENT EXCITATION FOR UNITY POWER FACTOR BQ Ğ 50O Z0-.1 + .3j V0 - .02 -.6 j 2iğ.1 +• .35 (Z - 1 -f- 2j) SYNCHRONOUS v OLTS moo x /AMP ROO 120C 1100 1000 .900. .800 .700. .600. .500. X X 550 ^ •i ^x LX "" ..... - — i — ğ. 70 / /^^ X ^ fiO A _* — ^,1 •*• _— - - j^~i' ^ x' -50L -40L t^ ^^ ^ / ——^£. ^ x^"^ 30 .150 100 50 / _*<^ x^ *<*" 20 / ^* ^ 10 ;. r i 0 2 0 £ 0 4 3 I o c 0 7 0 £ 0 S 0 1 30 1 .0 1 50 1 JO 1^ 10 IE 0 I 0 1 ron 0 1 )0 2 K> K' FIG. 26.—^Load curves of low-speed high-excitation induction motor con- verted to synchronous motor, at unity power-factor excitation. Converted to a synchronous motor, it has the constants: Synchronous impedance: Z = 0.1 + 1.97 j. Calculated in the same manner, the load curves, when vary- ing the f eld excitation with changes of load so as to maintain unity power-factor, are given in Fig. 26, and the load curves for constant field excitation giving a nominal induced voltage: e = L5 eo are given in Fig. 27. As seen, the increase of field excitation required to maintain