NASA's Jet Propulsion Laboratory, Pasadena, California
Sep 30 2001
These joints would be relatively compact, lightweight, simple, and inexpensive.
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The term "actuated ball-and-socket" (ABS) characterizes
a proposed class of ball-and-socket joints that would incorporate ultrasonic
motors and other piezoelectric actuators to generate multidimensional actuation.
In some applications, ABS joints could supplant traditional joint-and-actuator
assemblies that include passive rotary joints actuated by electromagnetic motors
via gears. In comparison with such assemblies, ABS joints offer potential advantages
of compactness, relative mechanical simplicity, higher torque-to-weight ratios,
no backlash, self-braking with power turned off, and lower cost. ABS joints
are expected to be particularly attractive for use as robot joints and as general
low-power orienting actuators for diverse applications that could include robot
hands, tools, and mechanisms for aiming scientific instruments.
Figure 1. Ultrasonically Vibrating Prods would be inserted in the ground,in a manner similar to that of a manaual search for mines. The robotic vehicle could also be equipped with an arm for digging up and removing mines.
Figure 1 illustrates an ultrasonic motor similar to those that would be included
in an ABS joint. This motor includes a washerlike rotor spring-loaded into contact
with a washerlike stator. The stator includes a ring of piezoceramic actuator
elements that are bonded to a base stator substructure, on the stator face opposite
that in contact with the rotor. The piezoceramic elements are positioned at
circumferential intervals and are electrically connected in alternating polarity.
When electrically excited by waveforms with a proper phase difference, the piezoceramic
elements deform in such a manner as to induce a wave that travels circumferentially
around the stator. This wave can be amplified by the resonance of the stator
and can have an amplitude of the order of several micrometers. As this wave
travels around the stator, it causes points on the free surface of the edge
of the stator to travel in small elliptical orbits. At crests of the wave, the
stator pushes against the rotor, so that through friction, some of the elliptical
motion is converted to rotary motion of the rotor.
Figure 2 depicts an ABS joint. A spherical rotor would fit in a housing that
would contain bearings. The housing would also contain three drive units (A,
B, and C) — each for rotation about one of three axes. These axes, which
span three-dimensional space, intersect at the center of the rotor. (The axes
are not necessarily perpendicular.) Power and control cables would be connected
to each drive unit.
Figure 2. Small Elliptical Orbital Motion of a point on the surface of the stator under the influence of a traveling wave causes (through friction) the rotor to move in a circumferential direction opposite that of the propagation of the wave
Within each drive unit, a thruster block would support an ultrasonic-motor
stator. This stator would likely be somewhat more complex than that of Figure
1: among other things, its rotor-contact surface would likely be spherical,
with a radius matching that of the rotor. Notwithstanding the added complexity,
the basic principle of operation would be the same as that of the ultrasonic
motor described above. By suitable electrical excitation of the stator, the
rotor could be made to rotate about the axis of symmetry of the drive unit.
A spring washer would push the thruster block, and thus the stator, radially
against the rotor. The rotor/stator friction associated with this radial preload
would establish the holding (braking) torque in the absence of applied power.
A piezoceramic ring, denoted the thruster, would be located between the thruster
block and a shelf in the housing. When not energized, the thruster would not
exert any effect. When electrically energized, the thruster would push the thruster
block radially outward (against the spring washer), thereby pulling the stator
out of contact with the rotor. Thus, energizing the thruster would prevent the
drive unit from either driving or braking the rotor.
To avoid working against the holding torque of the other drive units, only
one drive unit at a time could be used to produce rotation. For example, in
order to obtain rotation about axis A, it would be necessary to (1) excite the
stator of drive unit A with appropriately phased waveforms while (2) energizing
the thrusters of drive units B and C to prevent these units from braking the
rotation about axis A. To move the rotor from an initial orientation to a desired
final orientation, it would be necessary to generate a trajectory consisting
of a sequence of small rotations about the A, B, and C axes. It would be necessary
to develop an electronic data-processing and control system to compute and implement
the coordinated, sequential actuation of the three thrusters and the three ultrasonic-motor
stators to generate the trajectory. It has been estimated that, in a typical
application, the increments of rotation would be characterized by frequencies
of the order of a kilohertz.
This work was done by Issa Nesnas of Caltech for NASA's Jet Propulsion
Laboratory. For further information, access the Technical Support Package
(TSP) free on-line at www.nasatech.com
under the Machinery/Automation category.
NPO-20984
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