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220   Electric Drives and Electromechanical Systems


             where K is the stiffness at the rotor position under consideration and I tot is the sum of
             the motor inertia and the load inertia reflected back to the motor. The oscillating
             behaviour can be damped out, if required, for single-step operations by the use of
             mechanical (that is, viscous) or electrical damping. Excessive vibration of the
             mechanical system will result in wear, leading to premature mechanical failures.
                This resonance behaviour results in a loss of torque at well-defined stepping rates, as
             shown in the pull-out torque-speed characteristic in Fig. 8.6. These stepping rates can be
             determined from the natural frequency of the system, and they are given by,

                                               f n
                                            f k ¼  ðfor k ¼ 1; 2; . Þ                     (8.7)
                                                k
                Hence, if the motor and load have a natural resonance frequency of 120 Hz, the dips
                                                                    1
             in the speed-torque curve will occur at 40, 60, 120, steps s .


             8.4 Control of stepper motors
             The design of a drive system that incorporates a stepper motor should start with
             consideration of the steady-state performance; the choice of the type and step angle of
             the stepper motor is dictated largely by the maximum allowable positional error and by
             the maximum stepping rate which is required. While a stepper motor can be operated
             under either an open-loop or a closed-loop control system, this chapter will primarily
             discuss the open-loop approach. Closed-loop stepper-motor drives are no different
             from any other closed-loop drive, which are discussed in Chapter 10. Due to the
             inherent operation of a stepper motor, one change of phase excitation will result in the
             motor moving a specified, and accurately known, distance. The stepper motor’s
             position is controlled by generating a pulse train of known length, which is converted
             into the correct sequence of winding excitations by a translator, the winding power
             being switched by the drive circuit. A block diagram of a typical open-loop-stepper
             drive system is shown in Fig. 8.8. While the pulse generator and translator can be
             implemented in discrete logic, it is the current practice to use a microprocessor to
             control the whole process.
                During the design process, information is required on the restrictions that have to
             be placed on the timing of the pulse train to ensure satisfactory operation. These
             restrictions can be summarised as:
               The maximum step rate permitted for the required load torque. This can be deter-
                mined from the motor’s pull-out characteristic.
               The motor’s transient performance. If the load has a high inertia, the motor’s
                speed must be ramped up to ensure that the motor remains in synchronism with
                the step demand.
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