Actuators 21-63
Another practical example is a piezoelectric robot (Figure 21.85b), consisting of two spheres 1 and 2,
made from passive material (e.g., steel), with a piezoelectric transducer 3 between them. The contact
forces are ensured with the help of permanent magnet 4. Consisting of two spherical joints (two kinematic
pairs) the robot has up to 6 degree of freedom. The structure control and motions (rotations) in all
directions are achieved in the same manner as in the previous examples. The same active link is being
used here in two kinematic pairs to increase redundancy in the system. Using direct piezoeffect it is
possible to extract additional information (with the help of additional electrodes on the active link) on
the forces and torque, acting on the gripper and on the state of contacting surfaces. This information is
used to reduce positioning errors and to correct the motion trajectory.
References
Cady, W.G., Piezoelectricity, Dover publications, New York, 1964.
Volkov, V., Some theoretical problems in modern techniques of diagnostics in mechanical systems, in
Proc. Int. AMSE Conf. Systems Analysis, Control and Design, Lyon, France, 1994, pp. 205–212.
Williams, W. and Brown, W.J., Piezoelectric Motor, US Patent 2,439,499, 1942.
Ragulskis, K. and Bansevitchyus, R., Vibromotors – high frequency vibration motion converters, in Proc.
Int. Symp. Exploitation of Vibration, East Kilbridge, Glasgow, 1974, pp. 1–16.
Ragulskis, K. and Bansevicius, R., Vibromotors, Mokslas, Vilnius, 1981, (in Russian).
Ragulskis, K., Bansevicius, R. Barauskas, and G. Kulvietis, Vibromotors for Precision Microrobots, Hemi-
sphere Publishing Corporation, 1988.
Sashida, T. and Kenjo, T., An Introduction to Ultrasonic Motors, Oxford Science Publications, 1993, Oxford
University Press, New York.
Ueha, S. and Tomikawa, Y., Ultrasonic Motors, Theory and Application, Oxford Science Publications,
Oxford Press, Oxford, 1993.
Uchino, K., Piezoelectric Actuators and Ultrasonic Motors, Kluwer Academic Publishers, MA, 1997.
21.4 Hydraulic and Pneumatic Actuation Systems
Massimo Sorli and Stefano Pastorelli
21.4.1 Introduction
The primary function of an actuation system is to influence the controlled system so as to obtain the
desired movement or action. This objective is made possible by the actuation system, which converts the
primary energy with which the actuator operates into the final mechanical energy.
There are three main types of power with which actuation systems work: electric power, hydraulic
power, and pneumatic power. The first envisages the use of electric actuators such as motors, solenoids,
and electromagnets. The remaining two envisage the use of cylinders (linear motors) and rotary motors,
substantially similar in form and dimensions, the motion of which is respectively governed by a fluid
considered uncompressible in an initial approximation (a hydraulic liquid, mineral oil generally, or a
liquid with lower viscosity) and by a compressible fluid (compressed air or a generic gas).
Other types of energy are available but are fairly unusual in automatic systems. Chemical energy and
thermal energy, which cause a change of phase in a material or the thermodynamic expansion of the
systems into a mechanical movement, can be considered in this category.
The characteristics of fluid servosystems are examined below, with particular reference to systems
which permit continuous control of one of the two physical magnitudes which express the fluid power:
pressure and flow rate. In general, pressure control is carried out in cases in which it is necessary to create
a determined force or torque law, while flow rate control is used to carry out controls on kinematic
magnitudes such as position, speed, and acceleration.
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