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The outgassing rate for well-baked motors installed on a typical mechanism and run below 120 °C winding temperature is in
the order of 10-8 millibar litres sec-1. This represents high duty-cycle operation at rated phase current for size 35, 42 & 57
motors. The gas species are H2(90%) and CO (10%) and originate mainly from the windings and laminations. As a rule of
thumb, an additional 100 litres per second of pumping capacity per motor will be required for UHV. This gas load is insignificant
at HV and higher pressures.
14.3. Rotating Mechanisms Holding Torque
Design rotation mechanisms with balanced loads to reduce or eliminate the necessity for holding torque. If the torque imposed
on the motor by any imbalance of the load is less than the detent torque, then the motor will hold position without power.
The gearing required to achieve the desired angular resolution or to match the load inertia will increase the effect of detent
torque and also add friction.
14.4. Translation Mechanisms Shaft End-Float
The motor shaft has a compression spring, which pushes the shaft toward the mounting-face of the motor. The amount of
end-float is 100 to 200 µm for D35.1 and 200 to 400 µm for D42 motors. The spring is fully exercised with an axial force of 3 kg
toward the rear of the motor. For linear mechanisms where the motor is directly coupled to a leadscrew use gravity and/or
apply an opposite axial pre-load to avoid adding end-float to backlash.
There may be a significant static friction component added to the compression spring force, which may give the impression
that the end-float is less or that the spring is stiffer than specified. This should not be relied on to reduce backlash, as
repeatedly exercising the end-float will reduce the static friction and may also produce particles.
14.5. Resonances
Stepper motors are classic second-order systems and have one or more natural resonant frequencies. Operation at step rates
around these frequencies will excite the resonances, resulting in very low output torques and erratic stepping. The resonant
frequency is modified by the friction and inertia of the load, the temperature of the motor and by the characteristics of the
drive and therefore cannot be stated with any precision. Fortunately, coupling a load normally reduces the resonant
frequencies, which for unloaded AML motors occur below 300 Hz. The drive circuits of the SMD3 are optimised to produce
heavy damping of mechanical oscillations in the motors.
The simplest method of controlling resonances is to avoid operation of the motor close to the resonant frequencies. It is almost
always possible to start a motor at rates in excess of 400 Hz if the load inertia is matched as described in the next section.
Resonances are not usually a problem when the motor speed is accelerating or retarding through the resonance frequency
region.
If it is necessary to operate at slower speeds than this, the step division feature (micro-stepping) helps by effectively increasing
the stepping rate by the step division factor and reducing the amplitude of the step transients which excite the resonances. In
particularly difficult cases modifying the step frequencies at which transitions to micro-stepping occurs can be useful.
14.6. Load Inertia and Reduction Gearing
The load inertia coupled to the motor shaft should ideally be comparable to the rotor inertia of the motor where accurate
position control is required. The load inertia can be very much larger for speed control applications where some slip of
absolute position is unimportant. Where reduction gearing is used for load-matching the spur gear meshing with the motor
pinion will normally dominate the load inertia and it is important to keep its diameter small. Loosely coupled loads may give
rise to additional resonances at higher frequencies: these can usually be damped by substituting either anti-backlash or helical
gears in the gear train or arranging additional friction in the train.