Self-Locking Actuator for Hexapod Applications Combines High Push-Pull Force with Picometer Resolution for Active Optical Alignment in Astronomy

1. Introduction

Astronomical telescopes usually employ active position control for primary mirror surfaces using motorized mechanical actuators. The motion needed is generally quasistatic, to compensate gravitational and thermal effects. Another application for precision actuators within the telescope at a significantly faster motion response is the high speed tip/tilt control of a secondary or tertiary mirror.

Fig 1.1 shows a typical 6-axis hexapod positioner designed for secondary mirrors. It performs micron level positioning using high precision motorized components, and some designs have integrated piezoelectric actuators for rapid tip -tilt movements of the secondary mirror.

The classical design for a motorized actuator consists of a DC motor with an encoder, gears, and a leadscrew nut assembly to convert the rotary motion to linear translation. The achievable performance depends, for the most part, on the choice of mechanical components and the control algorithms. The physical size and mass of the actuation system is load dependent and for primary mirror applications often include counterbalancing mechanisms for offloading the motion drives. With high precision gears and leadscrews (e.g., Harmonic Drive gearheads, zero backlash ball, and roller screws) position resolutions of 0.1 to 0.5 µm can be achieved. The resolution can be bettered by adding a piggy-back piezo actuator with a high-resolution linear encoder, or by using motion deamplification techniques at the expense of added complexity and part count. All applications mentioned above require minimal energy consumption during operation for thermal control. An essential requirement then is that the units be self-locking when not under power, something which has required the addition of a brake acting on the leadscrew or motor for classical mechanical actuators. However, friction, play, and the associated manufacturing tolerances of the mechanical components limit the achievable position resolution in motorized actuator technology.

2. The Development of NEXLINE® Technology

Piezoelectric ceramic actuators however, acting as solid-state analog positioning elements, are not subject to these limitations. Piezo actuators can achieve extreme reliability and lifetime. An example is the NASA/JPL test of the PICMA® multilayer actuators form the Mars Mission. Here actuators were submitted to 100 billion cycles of life testing and survived without failures. For more information: Piezoelectric multilayer actuator life test and Precision Motion and Positioning Equipment on Mars Rover Curiosity – Still Going Strong.

The resolution of a piezo actuator is limited only by the noise on the control signal and is typically in the nanometer or picometer range. However, the displacement available with the piezo effect is limited to 0.1%-0.2% of the length of the piezo ceramics block. The implementation of piezo actuation to longer displacement (many millimeters) with high force has been very problematic over the years with vibrational/acoustic noise, low force, and low reliability from high wear rates as major technological hurdles. The motivation behind the development of NEXLINE® drives therefore was to provide the advantages of piezo actuators over long travel ranges while overcoming the technological hurdles mentioned above in a compact modular actuator.

2.1 Dither Mode Operation

A NEXLINE piezoelectric step drive consists of an arrangement of piezoelectric elements polarized in different directions. Shear piezo elements, highly preloaded against the runner, drive it perpendicular to the interface in a direction which depends on whether their control voltage is rising or falling. See Fig 2.2 and 2.2a.

In dither operating mode, all the drive piezos are operated in parallel and the stiffness and drive force can be scaled by increasing their number. Extremely high resolutions (picometer level) and high operating bandwidths can be achieved. However, the travel range available in this mode is limited from 5 to 8 µm, yet it is able to provide interferometric class position resolution for heavy optical surfaces or components.

2.2 Slew Mode Operation: Step and Constant Velocity Mode

In order to overcome the travel-range limitation of dither mode, each shear piezo is bonded to a longitudinal piezo which provides a clamp/unclamp effect. When a clamping piezo retracts, its shear piezo lifts off the runner. The clamping piezos are driven in two groups 180° out of phase. This makes it possible to combine short steps of the shear piezos into a longer move of the runner in either direction. See Fig 2.3.

Slew mode motion is divided into several different phases: Clamping piezos (group 2) unclamp, shear piezos (group 1) drive the runner forward while shear piezos (group 2) move backward, clamping piezos toggle, shear piezos (group 2) drive the runner forward while shear piezos (group 1) move backward. The available travel range therefore, can be scaled significantly with 10’s of millimeters as a normal range.

Slew mode motion begins and ends with zero control voltage on all piezo elements. This means that when powered down, the runner is held in place by the friction resulting from the high internal preload and can only be moved from its position by very high external forces.

In some applications, the discontinuities of the stepping motion described above can lead to undesirable oscillation of parts or assemblies. In such cases, it is possible for the slew mode controller to overlap the shear motion with the toggling of the clamping piezos, so that the piezos always clamp and unclamp the runner as it moves at a constant velocity. The operational compromise to obtain constant velocity slewing is lower force and step size compared to the full step slew mode.

2.3 Dynamic Park/Position Hold Mode

With the ability to slew and dither the Nexline actuator, another mode of operation can be realized. Upon a power off condition, the Nexline drive is programmed to remember it’s position, and by adjusting the voltage applied to the clamp and shear piezo actuators, it will hold it ’s exact position at the moment of the power off condition even as the PZT actuators discharge from their operating voltage to a zero volt condition.

This mode can also be implemented when the Nexline is in operation by commanding it to hold position while auto zeroing its bias voltage from programmed set points.  Maintaining an average low bias voltage greatly extends the operational lifetimes of the Nexline actuator since PZT ceramic lifetime is proportional to the average operating bias voltage.

3. Application

This technology was originally developed for applications in the semi -conductor industry. There, heavy, extreme precision optics assemblies, weighing 10’s of kg, must be positioned vertically and aligned in multiple axes with nanometer resolution. The coarse positioning requirements are for quasistatic motion over several millimeters to compensate for the relatively large mechanical tolerances in the manufacturing of machine components and structures. The fine positioning requirements, however, entail motion over a few microns with subnanometer resolution and sufficient bandwidth to also compensate for vibrational disturbances.

A significant requirement is that once on target, the position must be held with nanometer accuracy without having to apply voltage to the piezo elements. Fig 3.2 shows a linear actuator which meets the requirements listed above.

N-216 Operational Specifications:

• Up to 20 mm stroke
• 50 picometer resolution
• +/– 800 N ( 180 lb.) push/pull capability
• Actuator mass 1.2 Kg Actuator volume –340cc Stiffness – 45 N/micron
• Dynamic range over 2mm travel – >10,000,000

Also shown is a miniature version capable of 1.5 µm steps and forces to 50 N (see Fig 3.1).

In contrast to classical linear actuators, a number of components, such as leadscrew, gearbox, and bearings, can be dispensed with because the linear motion is generated directly. This makes it possible to realize very compact, low mass, high -load devices. Fig 3.3 shows a UHV-compatible hexapod made with fully nonmagnetic NEXLINE® actuators. Fig 3.4 shows a larger non-magnetic model for a complex alignment application involving superconducting magnets.