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    Design Tools   Catalogs   D757 – Escap® Ironless Rotor DC Micromotors and Step Motors

Escap® Ironless Rotor DC Micromotors and Step Motors

1.0 Introduction


This chapter on DC micromotors is intended as a tutorial review of the major engineering considerations required for the proper selection and application of ironless DC micromotors and tachometers. The text has been prepared for publication by Stock Drive Products with the permission of Portescap U.S.

2.0 Table of International Units and Conversion Factors Germane to Micromotor Applications


The International System of Units is used throughout this chapter, and Escap products are specified in this system of units. Consequently, the following tables have been prepared for the convenience the reader. A more complete treatment of the International System of Units and Conversion Factors is presented in the Designers Data Section of this handbook.

3.0 Advantages and Unique Features of an Ironless Rotor Motor

    Absence of Rotor Poles
  • no cogging (no preferred rotor position)
  • very low torque and back EMF variation with rotor position

    Small Rotor Inertia
  • rapid mechanical response

    Low Rotor Inductance
  • negligible electrical time constant
  • low torque ripple
  • low electrical noise
  • minimum brush/commutator electro-erosion

    Precious Metal Brush/Commutator System
  • negligible voltage drop at the brushes

    Negligible Hysteresis and Eddy Current Losses

    Very Stable Magnetic Field
  • very high over excitation to nonlinearity or demagnetization
  • low stray fields

    High Power to Volume Ratio
  • intense magnetic field
  • narrow air gap
  • high fill factor of copper conductor

    Continuous Copper Winding
  • excellent dynamic balance

    Low Internal Friction
  • tow starting voltage
  • low no-load current

    High Efficiency

    Good Compatibility with Simple Servo Drive Electronics

    Linear Characteristics


4.0 Construction of the Escap® Micromotor

4.1 General Construction and Geometry


Figure 1 shows the major subassembly breakdown of the motor. Brushes, housing, rotor and magnet are clearly shown. The primary feature is the self supporting "basket" construction of the rotor. In this geometry (Figure 2), the rotor is a perfectly wound (one conductor placed next to its neighbor without gap) surface of a right circular cylinder bonded to an insulating disc which supports the coil and commutator segments. The coil is wound in a unique skew configuration giving both electrical symmetry and mechanical stability. Precious- metal brushes and commutator are used to provide a near zero voltage drop, low friction and long life (Figure 3). Multiwire brush construction is employed to provide parallel contact redundancy.

Finally (Figure 4) the motor is assembled around a central permanent magnet and core which supports the bearings, outer magnetic return path and also the brush holder.


4.2 Stator-Housing Assembly


The stator consists of the central cylindrical permanent magnet, the core which supports the bearings, and the steel tube which completes the outer magnetic return path. All three of these parts are held together by the motor front plate, or the mounting plate. The magnetic core is magnetized diametrically after it has been mounted in the magnetic system. Owing to the low permeability of the permanent magnet, the magnetic resistance is great enough to allow neglect of the weakening of the stator field due to the rotor current.

4.3 Rotor Assembly


The ironless rotor, in the form of a cylinder, rotates around the magnetic core. In Escape motors, the rotor is made in the form of a skew wound coil and is fixed to a disc carrying the commutator. According to the motor dimensions, the commutator has between 5 and 13 segments. The small commutator diameter results in low sliding-speed and the small friction gives high efficiency. The perfectly symmetrical construction of the skew wound coil makes for smooth and silent running. The crossing of the wires makes the self supporting rotor winding (armature) highly stable mechanically.

4.4 Brush Holder End-Cap Assembly


The endcap includes the brush system. Owing to the use of precious metals for the brushes and the commutator segments, the low contact resistance of the brushes is maintained throughout the life of the micromotor and ensures starting at very low voltages.

4.5 d.c. Tachometers


The construction of the Escap® tachometer is identical to that of the motor. However, some engineering differences in the brush commutator system form the basic distinguishing features of the tachometer. The precious metals used for commutator and brushes have been selected to combine maximum life time with low noise performance. Unlike tachometers with carbon brushes, the use of precious metal brushes allows operation at very low currents (1 mA). Like any device with sliding mechanical contacts, the generator, under certain cir cumstances, may exhibit disturbances in the output signal of a very short duration (order of magnitude of 1 mS).

This in no way alters the rms value of the signal. in certain electronic circuits it may however be adviseable to provide a high resistance parallel path at the amplifier input or a simple filter circuit. The choice of the generator will essentially depend upon: Electronic considerations, such as desired value of signal and tolerated ripple, mechanical considerations, such as stresses on the shaft or resonance phenomena between generator and drive system.

We would add that the cleanliness of the signal depends to a large extent on the precise alignment of motor shaft and driven shaft, and that under severe conditions shielding of the tacho leads may be useful. The standard models are designed for operation at temperatures ranging from -30° C to +65° C (-20° F to +150° F); higher temperatures reducing the life of the sleeve bearings. Ball bearings are also available.

Every coil is switched twice per revolution, at the positive and negative brush. The ripple frequency per revolution is therefore twice the number of coils or number of commutator segments. The minimum peak-to-peak amplitude of ripple theoretically attainable depends upon the number of coils (which is always odd) and is
    4.89% for 5 coils
    2.51% for 7 coils
    1.52% for 9 coils
    1.02% for 11 coils
    0.73% for 13 coils
The actual value is largely determined by the precision of manufacture, primarily in coil winding.

image

image

typically generator output signal, 5 segment commutator a) value of the induced voltage(1 V) with actual ripple of 90 mV(9%)
b) (scale 10 times larger than a) minimum theoretical ripple, frequency per revolution equals twice the number of commutator segments.
c) actual ripple value, twice per revolution
d) signal for one complete revolution of rotor

 
Figure 5   Tachometer Output Signal



page 2 - Review of Physical Laws Governing Escap® Motor Applications