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Adjustable Speed Drive
Armature
Ball Bearing Motor
Brush
Brushed DC Motor
Brushless DC Motor
Commutator
DC motor
Direct Torque Control
Direct on Line Starter
Doubly-fed machine
ESC
Electrostatic Motor
Enameled Wire
Induction Motor
Inverter AC/DC
Linear Motor
Lynch Motor
Motor Controllers
Motor Soft Starter
Outrunner
Parvalux
Piezoelectric Motor
Repulsion motor
Shaded Pole Motor
Slip Ring
Squirrel-Cage Rotor
Stepper Motor
Traction Motor
Ultrasonic Motor
Vibrators
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Piezoelectric Motors
Piezoelectric motors are
made in both linear and rotary types.

Commonly known under the trademark names of Inchworm or PiezoWalk
motors, the most common type of piezoelectric motor uses three groups
of crystals: two of which are Locking and one Motive, permanently
connected to either the motor's casing or stator (not both) and
sandwiched between the other two, which provides the motion.
Current piezoelectric motors are fundamentally stepping motors, with
each step comprising either two or three actions, based on the locking
type.
Another mechanism employs the use of surface acoustic waves (SAW) to
generate linear or rotational motion.
A piezoelectric motor or piezo motor is a type of electric motor based
upon the change in shape of a piezoelectric material when an electric
field is applied. Piezoelectric motors make use of the converse
piezoelectric effect whereby the material produces acoustic or
ultrasonic vibrations in order to produce a linear or rotary motion.
In one mechanism, the elongation in a single plane is used to make a
series stretches and position holds, similar to the way a caterpillar
moves.
The non-powered behaviour of a piezoelectric motor is one of two
options: Normally Locked or Normally Free. When no power is being
applied to a Normally Locked motor, the spindle or carriage will not
move under external force. For a Normally Free motor, the spindle or
carriage will move freely under external force; However, if both
locking groups are powered at rest, a Normally Free motor will resist
external force without providing any motive force.
A combination of mechanical latches and crystals could be used, but
this would restrict the maximum stepping rate of the motor.
Stepping stages of Normally Free motorRegardless of locking type,
piezoelectric motors — both linear and rotary — use the same mechanism
to provide movement. First, one group of locking crystals is activated
— this gives one locked side and one unlocked side of the 'sandwich'.
Next, the motive crystal group is triggered and held — the expansion
of this group moves the unlocked locking group along the motor path.
This is the only stage where motor movement takes place.
Then the locking group triggered in stage one is released. Then the
motive group is released, retracting the 'trailing' locking group.
Finally, both locking groups are returned to their default states.
The growth and forming of piezoelectric crystals is a well developed
industry, yielding very uniform and consistent distortion for a given
applied potential difference. This, combined with the minute scale of
the distortions, gives the piezoelectric motor the ability to make
very fine steps — manufacturers claim precision to the nanometer
scale.
The high response rate and fast distortion of the crystals also allows
the steps to be made at very high frequencies — upwards of 5 MHz. This
gives a maximum linear speed of approximately 800 mm per second, or
nearly 2.9 km/h.
Piezo ratchet stepping motor. Very simple single-action stepping motors
can be made with piezoelectric crystals. For example, with a hard and
rigid rotor-spindle coated with a thin layer of a softer material
(like a polyurethane rubber), a series of angled piezoelectric
transducers can be arranged. When one group of transducers is
triggered, the rotor will be pushed around one step. This design is
not capable of such small or precise steps as more complex designs,
but can reach higher speeds and are cheaper to manufacture.
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