Piezoelectric flextensional actuators

In this project, I showed how to design and fabricate flextensional piezoelectric actuators on the millimeter scale with similar performance at high transmission ratios as their centimeter-scale counterparts. These actuators convert the large tensile stresses 25 Pa*m/V and small displacements (0.1% strain) generated via the converse piezoelectric effect into larger displacements at the expense of output force. The quality of this conversion, termed “mechanical efficiency”, is a key performance metric that I show how to optimize over five generations of actuator development, shown in the figure below. I provide simple guidelines based on lumped parameter modeling and scaling analysis to assist designers in sizing actuators to match specific size and output requirements.

cm laser scanner

This work enables new millimeter-scale systems and to facilitate the downscaling of existing centimeter-sized devices. These actuators can be used as building blocks in millimeter-sized devices in which precise, linear motion is needed, and the method of analysis employed should be broadly useful to designers of similar devices looking to distill a complex mechanics problem down to a set of simple design guidelines.

The potential applications for these devices on the millimeter scale are numerous, as judged by existing deployments in centimeter-sized systems. Claeyssen, et al. [1], describe a host of device applications: micro-scanning and shutter control for high-speed optical systems, active damping and shape control in aerodynamic systems, and acoustic sourcing for mapping underwater pipe networks and structural health monitoring. Janker, et al. [2] describe a wing morphing mechanism and vibration absorbers for helicopters and automobiles. Liu, et al. [3] and Lee, et al. [4] use flextensional actuators as the basis for in-plane and out-of-plane micropositioning stages, respectively.

Laser micromachining: This video shows the use of a galvo-operated UV laser to micromachine the carbon fiber amplification frame. This is the final step of device fabrication, in which the device is released from the multi-material laminate from which it is formed:

Free displacement: This clip shows the free (unloaded) motion of the actuator. For these type of devices, typical output displacements are ~50-100 um:

Blocked force: Next, this clip shows the other extreme of actuator performance: fully blocked output, in this case with a force sensor that allows the blocked force to be measured. Any internal motion of the actuator in this configuration represents loss in output work. Typical output force is ~50-100 mN:

Spring load: Lastly, this clip shows an intermediate loading condition: a spring load is attached to the output, and some intermediate force and displacement are achieved in between the extremes of free displacement and blocked force:

Microgripper demonstration: In this video, pincers are added to the flextensional actuator to enable grasping of small objects. This shows potential usage of this technology in micromanipulation applications:



References: [1] F. Claeyssen, R. L. Letty, F. Barillot, and O. Sosnicki, “Amplified piezoelectric actuators: Static & dynamic applications,” Ferroelectrics, vol. 351, no. 1, pp. 3–14, 2007.

[2] P. Janker, M. Christmann, F. Hermle, T. Lorkowski, and S. Storm, “Mechatronics using piezoelectric ¨ actuators,” Journal of the European Ceramic Society, vol. 19, no. 6, pp. 1127–1131, 1999.

[3] P. Liu, P. Yan, and Z. Zhang, “Design and analysis of an x–y parallel nanopositioner supporting largestroke servomechanism,” Proceedings of the Institution of Mechanical Engineers, Part C: Journal of Mechanical Engineering Science, vol. 229, no. 2, pp. 364–376, 2015.

[4] H.-J. Lee, H.-C. Kim, H.-Y. Kim, and D.-G. Gweon, “Optimal design and experiment of a three-axis out-of-plane nano positioning stage using a new compact bridge-type displacement amplifier,” Review of Scientific Instruments, vol. 84, no. 11, p. 115103, 2013.