EUCLID M2 MIRROR MECHANISM

Similar documents
GAIA M2M POINTING MECHANISM QUALIFICATION

CALIBRATION MECHANISM FOR INFRARED SPACE TELESCOPE. Patrice Kerhousse

TE 75R RESEARCH RUBBER FRICTION TEST MACHINE

Mounts for large lens in cooled environment

Piezoelectric Actuators and Future Motors for Cryogenic Applications in Space

RGS08 Linear Rails: RGS08 Non-Motorized With and Without Guide Screw. RGS08 Non-Motorized Linear Rails

LISA Telescope Assembly Optical Stability Characterization for ESA

THE EUCLID VIS READ-OUT SHUTTER UNIT: A LOW DISTURBANCE MECHANISM AT CRYOGENIC TEMPERATURE

RGS06 Linear Rails: RGS06 Non-Motorized With and Without Guide Screw. RGS06 Non-Motorized Linear Rails

Space mission environments: sources for loading and structural requirements

Selection Calculations For Linear & Rotary Actuators

SAMPLE CANISTER CAPTURE MECHANISM FOR MSR: CONCEPT DESIGN AND TESTING RESULTS INCLUDING 0-G ENVIRONMENT

Compact, lightweight, and athermalized mirror and mount for use on JWST's NIRCam instrument

LISA Telescope Assembly Optical Stability Characterization for ESA

Controlling Thermal Expansion

STRUCTURAL MODELS AND MECHANICAL TESTS IN THE DEVELOPMENT OF A COMMUNICATIONS SPACECRAFT

Control of the Keck and CELT Telescopes. Douglas G. MacMartin Control & Dynamical Systems California Institute of Technology

Coating K = TFE wear resist, dry lubricant Kerkote X = Special coating, (Example: Kerkote with grease)

SKF actuators available for quick delivery. Selection guide

RV SeRieS S P E C I F I C A T I O N S

Product Description. Further highlights. Outstanding features. 4 Bosch Rexroth Corporation Miniature Linear Modules R310A 2418 (2009.

A MIRROR CONTROL MECHANISM FOR SPACE TELESCOPE

E3000 High Power SADM Development

Product description. Compact Modules. Characteristic features. Further highlights

FORCE LIMITED VIBRATION TESTING OF CASSINI SPACECRAFT COSMIC DUST ANALYSER

Dynamic Tests on Ring Shear Apparatus

David Chaney Space Symposium Radius of Curvature Actuation for the James Webb Space Telescope

DISTRIBUTION LIST. Others original copies Name amount. Lens Research & Development 1x Uittenhout, J.M.M. 1x DOCUMENT CHANGE RECORD

THE SCANNING MECHANISM FOR ROSETTA / MIDAS FROM AN ENGINEERING MODEL TO THE FLIGHT MODEL

Dimensional stability testing in thermal vacuum of the CHEOPS optical telescope assembly

Introduction To Metrology

EXPERIMENTAL RESEARCH REGARDING TRANSIENT REGIME OF KINEMATIC CHAINS INCLUDING PLANETARY TRANSMISSIONS USED IN INDUSTRIAL ROBOTS

1990. Temperature dependence of soft-doped / hard-doped PZT material properties under large signal excitation and impact on the design choice

DESIGN AND QUALIFICATION OF THE CRYOGENIC COVER MECHANISM FOR THE MID-INFRARED INSTRUMENT ON THE JAMES WEBB SPACE TELESCOPE

Foundations of Ultraprecision Mechanism Design

Coupling System for Ultra Precision Machining

CTV series CHARACTERISTICS LINEAR UNITS

Precision Ball Screw/Spline

Development of Laser Thickness Gauge in Steel Plate Shearing Line

X-LRT-EC Series: High-load, closed-loop stages with built-in stepper motors, motor encoders, controllers, and dust covers

Expedient Modeling of Ball Screw Feed Drives

Analysis of a High-Precision Grinding Machine

x Contents Segmented Mirror Telescopes Metal and Lightweight Mirrors Mirror Polishing

Mirror Alignment and Optical Quality of the H.E.S.S. Imaging Atmospheric Cherenkov Telescopes

Development of a probe traversing system for an open test section wind tunnel

EQUIPMENT INTERFACE LOAD CHARACTERIZATION IN ACOUSTICS

Metrology Prof. Dr Kanakuppi Sadashivappa Bapuji Institute of Engineering and Technology Davangere

A deeper investigation into the thermal drift of a linear axis

3D metrology with a laser tracker inside a vacuum chamber for NISP test campaign

Design of a High Speed and High Precision 3 DOF Linear Direct Drive

New isostatic mounting concept for a space born Three Mirror Anastigmat (TMA) on the Meteosat Third Generation Infrared Sounder Instrument (MTG-IRS)

Linear guide drives. Synchronous shafts The use of synchronous shafts enables several linear axes to be operated with one drive.

Fine Alignment of the ATF Damping Ring

Revision 1.0, January 2014 MICRONIX USA, LLC

VST Project. M1floatation_VST-TRE-OAC Rel2.0. VST Project. Recovery Plan. M1 Floatation Support System

Inverted Pendulum System

R-Plus System Frontespizio_R_PlusSystem.indd 1 11/06/ :32:02

BUILDING LOW-COST NANO-SATELLITES: THE IMPORTANCE OF A PROPER ENVIRONMENTAL TESTS CAMPAIGN. Jose Sergio Almeida INPE (Brazil)

The basic dynamic load rating C is a statistical number and it is based on 90% of the bearings surviving 50 km of travel carrying the full load.

X-LSM-E Series: Miniature motorized linear stages with built-in motor encoder and controllers

November 3, 2014 Eric P. Smith JWST Program Office

(Refer Slide Time: 1: 19)

Tracker Tower 01 Prototype Test & Analysis Overview

Primary Mirror Cell Deformation and Its Effect on Mirror Figure Assuming a Six-zone Axial Defining System

New DCM for spectroscopy an engineering challenge review

X-LSM-SV1 Series: Low vacuum miniature motorized linear stages with built-in controllers

BRIGHT-STRATO SERIES

The Principles of Astronomical Telescope Design

New concept of a 3D-probing system for micro-components

SPICA/SAFARI (SPace Infrared telescope for Cosmology and Astrophysics)

Influence of electromagnetic stiffness on coupled micro vibrations generated by solar array drive assembly

High Power Electric Propulsion Pointing Mechanisms (HP EPPM) Technical Development Activities (TDA s) strategy, status and planning

Increasing of the Stern Tube Bushes Precision by On-Line Adaptive Control of the Cutting Process

MMT CONVERSION. Technical Report #31 SECONDARY MIRRORS SUPPORT. M2/F15 and M2/F9 HEXAPOD DESIGN. W. Gallieni, R. Pozzi

Space active optics: performance of Marie a deformable Laslandes mirror for. Devilliers, Arnaud Liotard, Céline Lopez, Frédéric Chazallet

INVESTIGATION OF BALL SCREWS FOR FEED DRIVE 1. INTRODUCTION

Manufacturing Equipment Control

The Silicon-Tungsten Tracker of the DAMPE Mission

LISA Pathfinder measuring pico-meters and femto-newtons in space

Picometre metrology. The Gaia mission will create an ultra-precise three-dimensional map of about one billion stars

TCS SERVO SYSTEM: Mechanical Modeling

Telescope Mechanical Design

GP-B Attitude and Translation Control. John Mester Stanford University

Development of the Screw-driven Motors by Stacked Piezoelectric Actuators

Physics 476LW Advanced Physics Laboratory Michelson Interferometer

SPICE SDM: INNOVATIVE APPROACHES FOR LINEAR MOTION AND HEAT MANAGEMENT

Measurement method for the proficiency testing program

Nanomotion Precision Piezo Ceramic Motors

ADM-Aeolus Science and Cal/Val Workshop

X-LRQ-SV2 Series: High vacuum motorized linear stages with built-in controllers

Technical Guide for Servo Motor Selection

Optical Method for Micro Force Measurement. Yusaku FUJII Gunma University

Objectives. Fundamentals of Dynamics: Module 9 : Robot Dynamics & controls. Lecture 31 : Robot dynamics equation (LE & NE methods) and examples

PETER: a double torsion pendulum to test quasi Free Fall on two Degrees of Freedom

OBSERVATIONS ON THE INFLUENCE OF LAUNCH VIBRATION ON BEARING TORQUE AND LUBRICANT PERFORMANCE

ROLLER BEARING FAILURES IN REDUCTION GEAR CAUSED BY INADEQUATE DAMPING BY ELASTIC COUPLINGS FOR LOW ORDER EXCITATIONS

The time period while the spacecraft is in transit to lunar orbit shall be used to verify the functionality of the spacecraft.

OWL: Further steps in designing the telescope mechanical structure and in assessing its performance

Rotary modules.

Modelling of a dynamic torque calibration device and determination of model parameters

Transcription:

EUCLID M2 MIRROR MECHANISM Aiala Artiagoitia (1), Carlos Compostizo (1), Laura Rivera (1) (1) SENER, Av. Zugazarte 56, 48930 Las Arenas (Bizkaia) Spain, Email: aiala.artiagoitia@sener.es ABSTRACT Euclid spacecraft is an ESA scientific programme whose main objectives is first to understand the origin of the Universe s accelerating expansion and secondly to probe the properties and nature of dark energy, dark matter, gravity from the measurement of the cosmic expansion history and the growth rate of structures. The focusing of the Euclid telescope is done on the M2 mirror which is installed on an orientation mechanism (M2MM). This mechanism shall accurately adjust the secondary mirror (M2) of the Euclid telescope to ensure the required optical quality in 3 degrees of freedom (translation in Z axis and rotations around X and Y axes). SENER is the contractor for the development of the mechanism and its driving electronics. This paper is prepared to explain the design and full test campaign of EUCLID M2MM Proto-Flight Model. Resolution, calibration and accuracy demonstration were performed at ambient temperature inside low humidity chamber using a robust set-up and optical encoders. As the mechanism does not include a hold down for launch, a good prediction of the structural behaviour is mandatory. The good correlation between predictions and the vibration tests results will be shown. The challenge during thermal vacuum (TV) test is to perform the functional performances test at 100K. The required test set up using interferometer and autocollimators to measure the six degree of freedom of the mirror movements will be presented. 1. INTRODUCTION The M2 Mirror Mechanism (M2MM) is a 3 degrees of freedom (dof) positioning mechanism which allows an accurate motion/adjustment of the secondary mirror (M2) of EUCLID telescope to ensure the required optical quality in orbit (recovery of misalignments of the telescopes due to the discrepancies between on-ground and in-orbit environments). The mechanism is based on the use of the actuator developed and successfully operated in orbit for GAIA mission. Mechanism design has been improved in view of the difficulties found in the GAIA mission: Full symmetrical arrangement of the actuators (the GAIA M2MM was not). Optimum stability and minimum excursion of the mirror position from assembly temperature at ambient up to operational one at 100K. The actuators position sensing is improved with the integration of two sensor for turns counting (mainly useful for on-ground testing). The mechanism is submitted to a complete test campaign. Difficulties and lessons learnt found for the demonstration of the performances and successful outcomes will be presented: Figure 1 EUCLID M2MM configuration 2. DESIGN REQUIREMENTS Main requirements of the mechanism: Overall stroke of mechanism is 400µm and +/- 1.5mrad Resolution shall be better than 0.1µm and 2.5µrad Accuracy shall be kept below ±3µm Withstand the mass of the mirror (3.1 kg) without a hold down device Full performances to be demonstrated at 100K Mechanism mass lower than 3.5 kg Proc. ESMATS 2017, Univ. of Hertfordshire, Hatfield, U.K., 20 22 September 2017

3. GENERAL M2MM CONFIGURATION The M2MM is the link between the optical bench and the secondary mirror and shall provide capability to adjust it in three dof, one translation and two rotations. The M2MM shall also maintain the position of the M2 mirror from the position defined during telescope alignment on ground, launch and in orbit transfer environment without any hold down device. The M2MM is composed of three linear actuators, which provide the desired three dof motion. The displacement in Z is obtained with the three actuators acting at same time. The two rotations are obtained by a differential linear displacement of the three actuator, which are placed in a triangular symmetrical arrangement. The joint between fixed interface (I/F) and tray and M2 mirror and tray is based on flexible elements. (called actuator input). The shaft pitch is 0.5mm. Linear resolution at motor-reducer output is 0.463µm/step. The flexure structure provides a reduction ratio from this linear movement of the output. As this reduction mechanism is variable, the output displacement is different for the same step increment. The reduction ratio varies from 12.4 to 8.1. Maximum resolution at actuator output is 0.057µm/step and minimum resolution at actuator output is 0.037µm/step. 4. GENERAL ACTUATOR CONFIGURATION The linear actuator for the EUCLID M2MM is a mechanism that provides 55nm resolution over a travel of 400µm with stable position at any point of the stroke. It also has high load capability to withstand launch loads without back driving. The different components of the actuator are basically: - A motor-reducer from CDA Intercorp, which includes a stepper motor and three stages gear reducer with a M3 thread spindle at output. - A symmetrical flexible structure, which includes two levers, two flexural joints or pivots, the output interface providing a reduction ratio and the I/F to fix to the M2MM tray. - A primary Vespel SP3 nut which joins the flexible structure via two blades to the spindle. - A secondary Vespel SP3 nut preloading the primary nut contact at any position within the stroke. - Two end stops at the beginning and end of the stroke for nut and blades protection and zeroing. - Two micro-switches one main and one redundant for turns counting. - A support structure where the motor-reducer and the top support of the spindle are mounted. Resolution at Motor-reducer and Actuator Level The selected stepper motor is a 6 pole motor (30 deg/step) with a reduction stage at the output of the motor of 90. Hence, rotational resolution at motorreducer output is 0.333deg/step. This motor actuates a spindle-nut, providing a linear displacement in the axis of symmetry of a mechanism Figure 2 Actuator Figure 3 Actuator main parts

Motorization Margin The motor torque capabilities shall be at least 2 time larger than the factorized resistive torques. Although most of the resistive torques are due to the loading of elastic elements where a factor of 1.2 is required, we have considered that all resistive torques are factorized by 1.5, and therefore, a total margin between the motor and the resistive torques of 3 had to be demonstrated. Actuator motorization torque has been measured via measurement of threshold current. It has been checked that the actuator moves with 1/3 of the motor torque capabilities without losing steps. The worst point of the stroke is close to the lower end stop, where the forces for deformation of the guides are maximum and the motorization margin minimum. The resistive force of the guides is maximum at 100K due to the increase of the Ti6Al4V stiffness. 5. EVOLUTION OF MECHANISM REQUIREMENTS AND PERFORMANCES One point of interest is to show the evolution of the mechanism requirements and performances from the mechanism developed for the GAIA mission. In Figure 4 is shown GAIA M2MM configuration to be compared with EUCLID M2MM, which is shown in Figure 5. Figure 5 EUCLID M2MM Table 1 shows the comparison of the main characteristics of the M2MM mechanism and actuator for GAIA and EUCLID missions. Perform. GAIA EUCLID M2 Mirror Mass 1.9 Kg < 3.1 Kg M2MM mass/qs <5.0 Kg / 30g <3.0 Kg / 28g First resonance frequency 128 Hz 161 Hz D.o.f. control 5 axes 3 axes Actuator Total Stroke +/- 315 µm +/- 220 µm Mechanism Op. Stroke Mechanism Resol. +/- 275 µm / +/- 2000 µrad < 0.06 µm / < 2 µrad +/- 200 µm / +/- 1500 µrad < 0.055 µm / < 2 µrad Op. Temp. 298K to 100K 298K to 100K Volume L 260 x W 110 x H 150 mm Hexagonal 214 mm /H 150 mm Position Accuracy < ±3 μm <± 40 μrad < ±3 μm <± 40 μrad Table 1 GAIA vs EUCLID M2MM performances Figure 4 GAIA M2MM (PFM) 6. EVOLUTION OF MECHANISM DESIGN Mechanism design has been improved in view of new requirements and difficulties found in GAIA mission: 1. Thermo-elastic stability: With respect to XY plane, the implemented solution has been performed via a symmetric design to guarantee that the interface point with the M2 mirror does not move with thermo-elastic deflection. With respect to Z axis, the distance between mirror and mechanism interfaces has been decreased to the minimum leading to minimum thermo-

elastic distortions from ambient to operation temperature. Figure 6 EUCLID M2MM with offloading devices 2. Three dofs instead of five dofs: The mechanism design is simplified by removing X and Y axes of movement. However, the drawback comes keeping the accuracy in X & Y axes having only the three Z axis actuators movements. Cross-talks displacements cannot be compensated. 3. Mass reduction: The mass of the mechanism is reduced to 3kg instead of 5kg. 4. Actuator sensors: They are implemented for on-ground purposes as a turn counter and since they are not allocated at 180º apart, the direction of rotation can be also known by noticing which one is switched on and off firstly with respect to the other. During functional tests it is verified the optimum repeatability of micro-switches activation. Figure 7 Micro-switches position into the actuator 7. PFM TEST CAMPAIGN The whole PFM test campaign includes: - CDA motor-reducer test at CDA premises - Repetition of individual CDA motor-reducer test at SENER premises - Actuator functional test (functional performances at ambient) - M2MM functional tests - M2MM vibration test - M2MM TV test. Thermal cycling and functional test at 100K. The major effort during the test campaign was dedicated to the functional performances verification. The final objective of the functional tests is to obtain the calibration curves for the kinematic model of the mechanism. Two were the major difficulties to be solved during functional tests, derived from the lubrication of the motor-reducer and the high resolution of the mechanism. Because of the MoS 2 lubrication of the motor-reducer ball bearings and gears, all the actuations of the mechanism and measurement at ambient conditions had to be performed in a humidity control chamber to prevent degradation of the lubrication. This limits the selection of the instrumentation, and makes more difficult the change between different configurations during testing. The high resolution of the mechanism requires a careful selection of the test instrumentation, compatible with restrictions imposed by the humidity control chamber and TV chamber, and able to measure the small displacements of the mechanism movement. Finally, for ambient measurements linear encoders were selected, whereas for vacuum measurements laser interferometers and autocollimators. Moto-reducer and Actuator tests The objectives of the test are: To measure the motor and actuator friction, and to verify motorization margin To check functional aspects such as stroke, repeatability, and end stops operation To verify telemetry All motor-reducer and actuator tests were done inside the humidity control chamber. The first step was to verify motor-reducer main requirements. Measurements are performed in two configurations using a DC external motor joined to a torquimeter and an angular encoder. Holding torque and internal frictions measurements are done from motor shaft, as can be seen in Figure 8.

Figure 8 Motor-reducer test from motor shaft The configuration shall be changed in order to measure motor-reducer backlash, back-driving and maximum torque. The DC external motor is joined to motorreducer output metric screw. The configuration of the set-up is changed inside the humidity control chamber, therefore, the motor-reducer is not exposed to ambient humidity. Figure 10 Actuator functional test Calibration curve and calculated error for one actuator are shown in Figure 11 and Figure 12 respectively. Figure 9 Motor-reducer test from output metric screw Once the motor-reducer is assembled with actuator pieces, functional aspects at actuator level are verified again. The main difficulty is to perform the adjustment of end stops and micro-switches inside the humidity control chamber as the motor-reducer must not run at ambient. Actuator stroke is measured using 2 linear optical encoders, one at each side of the actuator. Preliminary calibration curves are obtained to be used as baseline in whole mechanism functional test. Figure 11 Calibration curve Figure 12 Calculated error Functional Tests at Ambient The first functional tests were done at SENER facilities at room temperature, inside the humidity control chamber. In order to characterize the movement of the M2 mirror dummy, attached to the M2MM, six optical linear encoders were used. Figure 13 shows the test set-up with the encoders inside the humidity control chamber. With

this configuration, it was possible to measure the main movement of the mechanism (Z direction & X, Y rotations), and also the small translations and rotations in the other directions due to the cross-talk between axes. Figure 14 Micro-switches operation along the stroke Figure 13 Test set-up for measurement of movement inside the humidity controlled chamber One of the main objectives of this test was to measure the position of the mirror dummy for each step of the actuators. Therefore, optical encoders with 0.02µm resolution were selected, enough to achieve this goal. Temperature of the mechanism was continuously monitored during testing with thermocouples, in order to determine the influence of the temperature variations on the measurement of the position. The main objective of the test was to obtain calibration curves of the mechanism. The calibration curves are calculated via polynomial approximations. The position is measured accurately at several points along the stroke of the mechanism. This allows to stop the mechanism at desired points and to take a longer measurement for best filtering of the vibration. Six cycles are performed to obtain calibration curves. Calibration curves are calculated as polynomial approximations. The average of six cycles is used for polynomial curve calculation. These approximation curves will differ from the final ones obtained in vacuum with interferometer but they have to be obtained for the predictions of the movements required for the start of the functional tests at M2MM level in thermal chamber. Final approximation curves are obtained during TV tests at M2MM level. Resolution is calculated as the difference between two consecutive steps, and the polynomial approximation. Positioning error is the difference between calibration curve and measured data. During functional test it was also checked that microswitches are activated at every turn. Vibration Test The main goals of the vibration test were the following: - Determine the first natural frequencies. - Demonstrate the capability of the item to withstand the expected dynamic environment loads. - Demonstrate that actuators remain in the same position during vibration. The M2MM was tested assembled with dummy of the M2 mirror, as in Figure 15. Figure 15 M2MM with mirror dummy installed The M2MM was covered with a bag purged with 5X Nitrogen during vibration test in order to maintain ISO 5 cleanliness condition.

The main modes in each direction are summarised in Table 2, analysis data and measured data are compared: Mode Main direction Analysis data f [Hz] Measured data f [Hz] Diff. [%] 1 & 2 X & Y 165 161 2% 4 & 5 X & Y 309 320-4% 6 Z 341 336 1% Table 2 Main modes Figure 16 M2MM ready for vibration test The first resonance frequency of the M2MM was at 161Hz. During the test, it was also confirmed the good correlation between the predictions of the FEM and the results of the test, as can be appreciated in Figure 17 and Figure 18. Figure 17 FEM prediction for X-axis low level sine Figure 18 Test results for X-axis low level sine Sine qualification level vibration loads are up to 28g in the frequency range of 25Hz to 35Hz and 5g at 140Hz. As the first eigenfrequency (161Hz) is out the sine vibration frequency range, no notching is required during sine qualification level. Random qualification level are 17g RMS. The specified input is notched to 14g RMS in the fundamental global resonant frequencies, in order to limit the loads in the M2MM Interfaces. After the test, it was verified that the three actuators of the mechanism remained in the same position during vibration, maintaining the location of the M2 mirror dummy. The actuator is moved downwards and the micro-switches are activated at same step from upper end stop than one recorded during functional tests. Moreover, it was verified the correct performances of upper and lower end stops of the three actuators. Functional Thermal Vacuum Test Thermal vacuum cycling is performed at LINES laboratory at INTA facilities, including one nonoperational cycle between 333K and 100K, and three operational cycles between 323K and 100K. Functional tests will be performed at beginning and end of cycling, at 22ºC and at 100K, in order to measure the movement in 6 dof (Z translation, X & Y rotation, and cross-talks displacements and rotation) of the M2 mirror dummy at the top of M2MM. Functional tests at beginning of the cycling will be done to obtain the calibration curves of the mechanism. During the last cycle, functional test will be done to verify the pointing performance with the calibration curves obtained during the first cycle. The functional measurements at vacuum will be done with optical methods through two of the optical windows of the TV chamber. The following instrumentation will be used: - Three one-axis differential interferometers to measure translations along principal axes of the mechanism. - Two electronic autocollimators to measure rotations around principal axes of the mechanism.

There are two main problems for measuring accurately the position: the vibration of the mechanism and thermal effects. The main contribution to the vibration is the thermal vacuum chamber and cooling system. Regarding the thermal effects, the temperature of the M2MM is quite well controlled inside the chamber. These factors are especially unfavourable for the measurements of translations, so as to minimize its impact, two optical cubes will be used: one mobile on the M2 mirror dummy, and one fixed (close to the other) on the test jig to be use as reference for interferometers (see Figure 19). This reference improves significantly the noise and the stability of the measurement of the translations; however, it also increases the difficulty of the alignment of the optical instrumentation. been faced by SENER during the design and test phases of the EUCLID M2MM. The main design issues were to reduce the thermal loads with a symmetrical design and to reduce thermo-elastic excursion from ambient to 100K. It must be highlighted the difficulty found during test campaign due to the high resolution of the mechanism and the constraints regarding environmental conditions during functional testing. 9. ACKNOWLEDGEMENTS We would like to thank the LINES team at INTA, especially Tomás Belenguer and Gonzalo Ramos, for their fundamental contribution to the success of the project, performing the optical measurements to verify the functional performances of the mechanism during thermal vacuum testing. 10. REFERENCES 1. Compostizo, C., Lopez, R. & Rivera, L. (2011). GAIA M2M Pointing Mechanism Qualification. ESMATS 2011. Figure 19 M2MM ready to install in TV chamber The purpose of the test is to obtain calibration curves and to verify the torque margin at 100K. Calibration curves are obtained as polynomial approximations. Same procedure as in ambient functional test is used for calibration curves calculation. Positioning error also appears in the measurement in vacuum, as the difference between calibration curve and measured data. The calibration curves obtained during the first thermal cycle will be verified during the last one. In this test, the M2MM is commanded to achieve a set of positions moving the three actuator together with their calibration curves, covering the full range in the three dof of the mechanism. For each position in the set, the error is computed as the difference between measured position and target one. 8. CONCLUSIONS The EUCLID M2M mechanism is based on the use of the actuator developed and successfully operated in orbit for GAIA mission. However, several challenges have