Figure 1 - Typical inductance profile plotted against
, for
each phase of a two phase stepper motor.
It can be seen on Figure 1 that in no time the inductance
falls to zero. Torque generated by such a motor is given by:
=
2 ∙
()
(1)
where
is the current on the winding,
(θ)
is the inductance
of the phase and
is the angular position of the shaft.
Figure 2 presents the torque generated by the previously
described stepper motor and such waveform is obtained by
taking the derivative of inductance with respect to
. It
should be noted that magnetic saturation effect was not
considered.
Figure 2 - Typical torque exerted by a two phase stepper
motor.
The behavior seen in Figure 2 justifies why stepper motors
are inherently used for position control: when a given
winding is energized, the rotor aligns with the respective
stator energized winding; if some external load torque tries to
move the rotor from that position, an opposing torque will
act in such a way to move back the rotor to the original rest
position; if the load torque is higher than any opposing
torque that the motor can generate, the shaft will enter an
instability region and will move the rotor to another stable
position.
From Figures 1 and 2, it can be seen that stepper motors'
resolution is related to its mechanical complexity, in a sense
that the smaller distance between peeks for an inductance
waveform, the higher will be its mechanical resolution.
General purpose motors, with cylindrical rotor, the resolution
can be as low as 0.9˚. Application specific motors, with disk
rotor structure, resolution can be as low as 0.05˚.
From that previous analysis, it can be observed that to
control the position of a stepper motor, one only have to keep
a constant current flowing through a stator winding.
However, this position control is limited by three elements:
its maximum torque driving capacity, known as holding
torque; the number of phases a motor has; and the number of
tooth that both stator and rotor have.
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