Page 621 - Mechatronics with Experiments
P. 621

ELECTRIC ACTUATORS: MOTOR AND DRIVE TECHNOLOGY  607
                                  During acceleration, a motor adds mechanical energy to the load. It acts as a motor.
                             During deceleration, the motor takes away energy from the load. It acts like a brake
                             or generator. This means that energy is put into the load inertia during acceleration, and
                             energy is taken from the load inertia (returned to the drive) during deceleration (Figure 8.2).
                                  Some drives can convert the generated electric power and put it back to into the
                             electric supply line while others dump the regenerative energy as heat through resisitors.
                             The amount of regenerative energy depends on the load inertia, deceleration rate, time
                             period, and load forces.
                                  There are two different motion conditions where regenerative energy exists and
                             satisfies the T ⋅ w < 0 condition:

                                1. During deceleration of a load, where the applied torque is in the opposite direction
                                  to the speed of inertia.
                                2. In load driven applications, that is in tension controlled web handling applications, a
                                  motor may need to apply a torque to the web in the opposite direction to the motion
                                  of motor and web in order to maintain a desired tension. Another example for this
                                  case is where the gravitational force provides more than the needed force to move an
                                  inertia, and the actuator needs to apply force in the direction opposite to the motion
                                  in order to provide a desired speed.

                             Example     Consider the electric motor driven load shown in Figures 8.3 and 8.4. Assume
                             that the load is a translational inertia and an electric motor is a perfect linear force generator.
                             Consider an incremental motion that moves the inertia from position x to position x using
                                                                                                2
                                                                                     1
                             a square force input. For simplicity, let us neglect all the losses. We will assume that the
                             motor-drive combination converts electrical power (P (t)) to mechanical power (P (t))
                                                                                                 m
                                                                         e
                             with 100% efficiency in the motoring mode, and mechanical power to electrical power with
                             100% efficiency in the generator mode.
                                                            P (t) = P (t)                        (8.4)
                                                             e
                                                                   m
                                                            DC bus



                                                                                              Load
                                                            R regen  C cap                    x
                               3 Phase
                             AC source                                               M           m
                                                                                             F







                                             Rectifier                   Inverter





                                                   Non–regenerative  Regenerative drives
                                                      drives
                                                     R   ≠ 0           R regen  = 0
                                                      regen
                             FIGURE 8.3: Regenerative energy in motion, its storage and dissipation.
   616   617   618   619   620   621   622   623   624   625   626