Page 680 - Mechatronics with Experiments
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666   MECHATRONICS
                                   It should be quickly pointed out that these performance characteristics are only for the
                              motor when controlled from a line voltage supply directly without any active commutation
                              by a drive. The current-torque characteristics of an AC motor can be made to behave like
                              a DC motor using the so called “field oriented vector control” algorithm which is typically
                              implemented in the drive. The performance of a motor should always be evaluated together
                              with the drive it is used in. Depending on the drive type used, the performance characteristics
                              of the motor-drive combination can be quite different.

                              Example    Consider an AC induction motor driven by a line supply frequency of w =
                                                                                                   e
                              60 Hz. Assume that it is a two-pole motor, P = 2. The motor design is such that at the
                              maximum load, the slip is 20% of the synchronous speed, s = 20%. Determine the speed
                              of the motor for the following conditions: (a) no-load speed, (b) speed at maximum load,
                              (c) speed at a load that is 50% of the maximum load. Determine the speed variation
                              (sensitivity) due to the variation of load as percentage of its maximum value. Let maximum
                              load torque be 100 lb ⋅ in.
                                   Referring to Figure 8.41, let us assume that the curve connecting the no-load speed
                              and maximum-load speed points is a linear line. In steady-state, the actual motor speed is
                              determined by the intersection of the torque-speed curve with the load torque. As long as
                              the load torque is less than the maximum load torque, the motor speed will be somewhere
                              between the no-load speed and the speed at maximum load. As the load varies up to the
                              maximum load torque, the steady-state speed of the motor variation follows the linear
                              torque-speed line.
                                   The no-load speed of the motor is
                                                    w e   60 Hz
                                              w rm  =   =      = 60 rev∕s = 3600 rev∕min        (8.250)
                                                    P∕2    2∕2
                              At the maximum load, the motor specifications indicate that it has 20% slip,
                                                  w syn  − w rm
                                               s =          = 0.2                               (8.251)
                                                     w
                                                      syn
                                             w  = w   − 0.2 ⋅ w  = 0.8 ⋅ w  = 2880 rev∕min      (8.252)
                                              rm    syn      syn       syn
                              When the load is 50% of maximum load, the slip will be 50% of the maximum slip.
                              Therefore, the steady-state rotor speed is
                                                   w syn  − w rm
                                               s =          = 0.1                               (8.253)
                                                     w syn
                                             w rm  = w syn  − 0.1 ⋅ w syn  = 0.9 ⋅ w syn  = 3240 rev∕min  (8.254)

                              The speed varies from synchronous speed at no-load to 20% slip at maximum load, hence
                                                            w   − ((1 − s) ⋅ w  )
                                                      ΔV     syn           syn
                                                          =                                     (8.255)
                                                      ΔT           100
                                                         l
                                                            s ⋅ w syn
                                                          =                                     (8.256)
                                                             100
                                                          = 7.2rpm∕(lb ⋅ in)                    (8.257)

                              8.5.2 Drives for AC Induction Motors
                              The drive controls the electrical variables, which are the voltage and current, in the stator
                              windings of an AC induction motor in order to obtain the desired behavior in mechanical
                              variables, which are torque, speed, and position. In particular, frequency and magnitude
                              of the voltage control are of interest. Major drive types are discussed below (Figure 8.43)
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