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ECONOMICAL STEPPER MOTORS FOR SPEED-CONTROL APPLICATIONS


                  Indexing terms:   Stepping motors, Velocity control

                  Abstract: It is shown that automobile alternators can provide a low-cost alternative to a conventional stepper
                  motor in speed-control applications. Typical performance curves using a transistorised inverter are provided.


Introduction: Stepper motors are widely used in industry,                  Measured line voltages and line currents at different
and elsewhere, for two principal purposes;position control              motor speeds are shown in Fig. 2. At low speeds the current
and speed control. To these ends a wide variety of motors               waveform has the expected form while, at higher speeds,
differing in step size, speed, drop-out torque and cost have            more distortion is present. As discussed by Tal3 this
been developed and marketed. In general the emphasis has                 constant-current excitation maximises the output power
been on higher resolution at the expense of speed and cost.             for a given thermal dissipation in the motor. These wave-
Such motors are ideal for operating machine tools and                   forms, although distorted, are closer approximations to
other applications where an accurate position must be                   sinusoidal currents than square waves and give close to
maintained for some process time and then changed.                      optimal performance.
    In many applications, however, these motors, while                     In practice, with a 25—40 V d.c. busbar, constant motor
suitable, are overdesigned for the purpose. For example,                currents of 10 A can be achieved with d.c. busbar currents
in chemical plants a constant rate of flow through some                 of the order of 3—2 A when the motor is unloaded. At
positive-displacement pump requires a constant-speed                    higher loads the d.c. current and the maximum line current
motor. The step size is, in this case, largely irrelevant, and          tend to become more equal. The exact ratio between these
significant savings in cost can readily be achieved using               currents depends on the d.c. busbar voltage, the inverter
lower-resolution motors. Such motors are not usually                    switching speed and efficiency, the motor core and I2R
available from traditional stepper-motor sources, but                   losses, and the mechanical load.
automobile alternators have been found to be extremely                     Performance curves for a typical automobile alternator
useful and almost universally available. They are available             used as a stepper motor driven with a constant current
with power ratings up to ~ 1 kW at much lower cost than                 transistorised inverter are shown in Fig. 3. In this case the
conventional stepper motors.                                            maximum power output is 180 W at 1800 r/min. The motor
                                                                        has a useful holding torque of 1 -3 Nm and a maximum
 Description and results: Automobile alternators are usually            speed of 2500 r/min. Higher d.c. busbar voltages are
star-connected 3-phase machines with, commonly, 8 or 12                 effective in increasing the maximum speed and higher
poles giving 24 or 36 equivalent steps/revolution. To                   (constant) currents increase the holding torque.
modify an automobile alternator for use as a stepper motor
it is only necessary to disconnect the rectifier stack and                      d.c. busbar «•
connect a 3-phase inverter directly to the stator windings.
Rotor excitation is conveniently provided using the slip
rings on the machine. In explosion-critical environments
such external rotor excitation can be dispensed with by
replacing the rotor winding with toroidal permanent
magnets on a (new) nonmagnetic shaft.
    A suitable inverter configuration is shown schematically                                             ^® A
in Fig. 1. In essence this inverter is less complex than that
required for a 2- or 4-phase system, as it only requires three
'totem-pole' drivers. Following Nagasaka and Shinohara,1                   current
constant current excitation has been used, but the                         select /control
implementation, in this case, is rather novel as it uses the
inductance of the motor in conjunction with the flywheel
diodes and transistors as a high-efficiency switching
regulator.
   Transistors 1—6 are switched in the usual 'quasi-square-
wave' or '6-step' sequence described by Miller and
Lawrence.2 The three currents to the motor are monitored                Fig. 1 Schematic diagram of transistorised inverter
using electronic ammeters / , , / 2 , and / 3 . The magnitude           Transistors Tl — Tf are any suitable switching transistor (e.g. 2N305 5)
of the largest current is selected, and, if this magnitude is           The diodes should be fast soft recovery types
above a predetermined level, the whole inverter is turned
off until the current drops to slightly below that level.
Switching the inverter off and on is accomplished by simply              Conclusions: Automobile alternators are ' designed to
switching whichever of transistors 2, 4, or 6 are active in             operate over a wide range of conditions in a very hostile en-
the 6-step sequence. The hysteresis in the current level at             vironment. When they are used as stepping motors they
which switching occurs is chosen to ensure that the on/off              still have these performance characteristics. Coupled with
switching rate is kept well into the ultrasonic area where it           this ruggedness the lower cost of an automobile alternator
is not aurally objectionable.                                           often means that a complete stepper-motor system (motor

ELECTRIC POWER APPLICATIONS, FEBRUARY 1979, Vol. 2, No. 1                                                                                    27
                                                                                                       0140-1327/79/010027 + 02 $01-50/0
plus inverter) can be made for less cost than the equivalent
                                                                 stepping motor alone.

                                                                                                                          l200




                                                                                500       1000     1500        2000    2500
                                                                                             speed, r/min

                                                                 Fig. 3 Measured torque and power characteristics of a typical
                                                                 automobile alternator type BOSCH 14 V, 35 A (G.M. part number
                                                                 9929209)
                                                                 Rotor excitation 2 A d.c., busbar voltage 40 V
                                                                 Inverter constant current setting 7 A



                                                                 J.T. BOYS                           25th September 1978
                                                                 Department of Electrical Engineering
                                                                 University of Auckland
                                                                 Auckland
                                                                 New Zealand

                                                                 G.R. DUNLOP

                                                                 Department of Electrical Engineering
                                                                 University of Canterbury
                                                                 Christchurch
                                                                 New Zealand



                                                                  References

                                                                  1 NAGASAKA, M., and SHINOHARA, K.: 'A study of large
                                                                    capacity electric pulse motors', Electr. Eng. Jpn., 1974, 94, pp.
                                                                    101-109
Fig. 2 Measured line voltages and line currents for a typical     2 MILLER, D.W., and LAWRENCE, R.G.: 'Variable-frequency
automobile alternator at different speeds                           inverter and its application to motor drives', Electron. & Power,
Upper 60 r/min. middle 300 r/min, lower 1200 r/min                  1976, 22, pp. 675-678
The d.c. busbar is an unregulated supply of 40 V                  3 TAL, J.: 'Control modes of step motors', IEEE Trans., 1977,
All current waveforms (upper traces) are 7 A peak                   AES-13, pp. 56-61

                                                                                                                           T284P




 28                                                             ELECTRIC POWER APPLICATIONS, FEBRUARY 1979, Vol. 2, No. I

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Economical stepper motor

  • 1. Correspondence ECONOMICAL STEPPER MOTORS FOR SPEED-CONTROL APPLICATIONS Indexing terms: Stepping motors, Velocity control Abstract: It is shown that automobile alternators can provide a low-cost alternative to a conventional stepper motor in speed-control applications. Typical performance curves using a transistorised inverter are provided. Introduction: Stepper motors are widely used in industry, Measured line voltages and line currents at different and elsewhere, for two principal purposes;position control motor speeds are shown in Fig. 2. At low speeds the current and speed control. To these ends a wide variety of motors waveform has the expected form while, at higher speeds, differing in step size, speed, drop-out torque and cost have more distortion is present. As discussed by Tal3 this been developed and marketed. In general the emphasis has constant-current excitation maximises the output power been on higher resolution at the expense of speed and cost. for a given thermal dissipation in the motor. These wave- Such motors are ideal for operating machine tools and forms, although distorted, are closer approximations to other applications where an accurate position must be sinusoidal currents than square waves and give close to maintained for some process time and then changed. optimal performance. In many applications, however, these motors, while In practice, with a 25—40 V d.c. busbar, constant motor suitable, are overdesigned for the purpose. For example, currents of 10 A can be achieved with d.c. busbar currents in chemical plants a constant rate of flow through some of the order of 3—2 A when the motor is unloaded. At positive-displacement pump requires a constant-speed higher loads the d.c. current and the maximum line current motor. The step size is, in this case, largely irrelevant, and tend to become more equal. The exact ratio between these significant savings in cost can readily be achieved using currents depends on the d.c. busbar voltage, the inverter lower-resolution motors. Such motors are not usually switching speed and efficiency, the motor core and I2R available from traditional stepper-motor sources, but losses, and the mechanical load. automobile alternators have been found to be extremely Performance curves for a typical automobile alternator useful and almost universally available. They are available used as a stepper motor driven with a constant current with power ratings up to ~ 1 kW at much lower cost than transistorised inverter are shown in Fig. 3. In this case the conventional stepper motors. maximum power output is 180 W at 1800 r/min. The motor has a useful holding torque of 1 -3 Nm and a maximum Description and results: Automobile alternators are usually speed of 2500 r/min. Higher d.c. busbar voltages are star-connected 3-phase machines with, commonly, 8 or 12 effective in increasing the maximum speed and higher poles giving 24 or 36 equivalent steps/revolution. To (constant) currents increase the holding torque. modify an automobile alternator for use as a stepper motor it is only necessary to disconnect the rectifier stack and d.c. busbar «• connect a 3-phase inverter directly to the stator windings. Rotor excitation is conveniently provided using the slip rings on the machine. In explosion-critical environments such external rotor excitation can be dispensed with by replacing the rotor winding with toroidal permanent magnets on a (new) nonmagnetic shaft. A suitable inverter configuration is shown schematically ^® A in Fig. 1. In essence this inverter is less complex than that required for a 2- or 4-phase system, as it only requires three 'totem-pole' drivers. Following Nagasaka and Shinohara,1 current constant current excitation has been used, but the select /control implementation, in this case, is rather novel as it uses the inductance of the motor in conjunction with the flywheel diodes and transistors as a high-efficiency switching regulator. Transistors 1—6 are switched in the usual 'quasi-square- wave' or '6-step' sequence described by Miller and Lawrence.2 The three currents to the motor are monitored Fig. 1 Schematic diagram of transistorised inverter using electronic ammeters / , , / 2 , and / 3 . The magnitude Transistors Tl — Tf are any suitable switching transistor (e.g. 2N305 5) of the largest current is selected, and, if this magnitude is The diodes should be fast soft recovery types above a predetermined level, the whole inverter is turned off until the current drops to slightly below that level. Switching the inverter off and on is accomplished by simply Conclusions: Automobile alternators are ' designed to switching whichever of transistors 2, 4, or 6 are active in operate over a wide range of conditions in a very hostile en- the 6-step sequence. The hysteresis in the current level at vironment. When they are used as stepping motors they which switching occurs is chosen to ensure that the on/off still have these performance characteristics. Coupled with switching rate is kept well into the ultrasonic area where it this ruggedness the lower cost of an automobile alternator is not aurally objectionable. often means that a complete stepper-motor system (motor ELECTRIC POWER APPLICATIONS, FEBRUARY 1979, Vol. 2, No. 1 27 0140-1327/79/010027 + 02 $01-50/0
  • 2. plus inverter) can be made for less cost than the equivalent stepping motor alone. l200 500 1000 1500 2000 2500 speed, r/min Fig. 3 Measured torque and power characteristics of a typical automobile alternator type BOSCH 14 V, 35 A (G.M. part number 9929209) Rotor excitation 2 A d.c., busbar voltage 40 V Inverter constant current setting 7 A J.T. BOYS 25th September 1978 Department of Electrical Engineering University of Auckland Auckland New Zealand G.R. DUNLOP Department of Electrical Engineering University of Canterbury Christchurch New Zealand References 1 NAGASAKA, M., and SHINOHARA, K.: 'A study of large capacity electric pulse motors', Electr. Eng. Jpn., 1974, 94, pp. 101-109 Fig. 2 Measured line voltages and line currents for a typical 2 MILLER, D.W., and LAWRENCE, R.G.: 'Variable-frequency automobile alternator at different speeds inverter and its application to motor drives', Electron. & Power, Upper 60 r/min. middle 300 r/min, lower 1200 r/min 1976, 22, pp. 675-678 The d.c. busbar is an unregulated supply of 40 V 3 TAL, J.: 'Control modes of step motors', IEEE Trans., 1977, All current waveforms (upper traces) are 7 A peak AES-13, pp. 56-61 T284P 28 ELECTRIC POWER APPLICATIONS, FEBRUARY 1979, Vol. 2, No. I