Page 137 - Handbook of Electrical Engineering
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INDUCTION MOTORS     119


           R 22N , X 22N , R 33N and X 33N . The cycle is repeated using the ‘old’ values (call these R 22O , X 22O , R 33O
           and X 33O ) plus a small amount of the error between the ‘new’ and ‘old’ values, i.e.,

                                        R 22 = R 22O + k(R 22N − R 22O )
                                        X 22 = X 22O + k(X 22N − X 22O )
                                        R 33 = R 33O + k(R 33N − R 33O )

                                        X 33 = X 33O + k(X 33N − X 33O )

                 The value of ‘k’ should be chosen to be between +0.001 and +0.01 to ensure stability. The
           process is stopped once the absolute error in each of the parameters has fallen below a suitably small
           value, e.g. 0.001 per-unit of its absolute value. Tables 5.9 and 5.10 for two-pole induction motors
           were complied from Tables 5.1, 5.2, 5.5 and 5.6, to show the results of the method.


           5.3 CONSTRUCTION OF INDUCTION MOTORS

           The physical construction of an induction motor is greatly influenced by the environment and ambient
           conditions. The environmental conditions include considerations for explosion, corrosion, dampness,
           ingress of dust and solid particles, proximity to human operators, cost and economics. Ambient con-
           ditions relate to surface temperature, methods of cooling, fan design and appropriate derating factors.

                        Table 5.9.  Per-unit resistances for equivalent double-cage two-pole motors

                     Rated power    Slip (pu)    R 20      R 21       R 22      R 33
                     (kW)
                          LV          —          —         —          —          —
                          11        0.0433     0.0323     0.0398    0.0434     0.11308
                          15        0.0355     0.0270     0.0411    0.05127    0.05491
                          22        0.0282     0.0218     0.0421    0.05865    0.03391
                          30        0.0237     0.0186     0.0425    0.06165    0.02619
                          37        0.0216     0.0167     0.0425    0.06342    0.02232
                          45        0.0191     0.0152     0.0423    0.06389    0.01967
                          55        0.0173     0.0138     0.0419    0.06402    0.01737
                          75        0.0150     0.0120     0.0410    0.06378    0.01461
                          90        0.0138     0.0111     0.0403    0.06312    0.01332
                         110        0.0126     0.0103     0.0393    0.06210    0.01222
                         132        0.0117     0.00955    0.0384    0.06119    0.01120
                         160        0.0108     0.00888    0.0372    0.06007    0.01032
                         200        0.00995    0.00820    0.0357    0.05840    0.00945
                         250        0.00917    0.00759    0.0341    0.05685    0.00868
                         315        0.00846    0.00705    0.0323    0.05485    0.00802
                         HV           —          —         —          —          —
                         630        0.00887    0.00771    0.0183    0.03660    0.00920
                         800        0.00896    0.00776    0.0175    0.03491    0.00995
                        1100        0.00901    0.00777    0.0172    0.03587    0.00989
                        2500        0.00883    0.00740    0.0205    0.06099    0.00841
                        5000        0.00842    0.00672    0.0303    0.12957    0.00709
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