implications of wind testing results on the gsmt control systems

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Implications of Wind Testing Results on the GSMT Control Systems. David R. Smith MERLAB, P.C. Hierarchical Approach. If errors can be arranged hierarchically, then the control system can be as well. Large, high payload, long stroke systems can be slow and less precise. - PowerPoint PPT Presentation

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Implications of Wind Testing Results on the GSMT Control

Systems

David R. Smith

MERLAB, P.C.

Hierarchical Approach

• If errors can be arranged hierarchically, then the control system can be as well.

• Large, high payload, long stroke systems can be slow and less precise.

• Higher bandwidth systems can be smaller stroke and capacity.

Hierarchical Approach (cont.)

• Keeping high-bandwidth control on smaller systems eliminates control-structure interactions.

• Intent is to keep cost/risk low by combining simpler and more standard control systems and components.

Errors• Large, slow errors (m-mm, <0.01-0.1 Hz)

– Gravity– Thermal– Mechanical misalignments– Wind

• Medium-sized, rate (<~10 m, <~10 Hz)– Wind– Vibrations

• Small, fast errors (<1 m, >~10 Hz)– Wind– Vibrations– Atmosphere

Controllers (example)

• Main Axis

• M1 Gross/Fine Position

• M1 Segment warping

• M2 Positioner

• M2 Fast tip/tilt/position

• M2 Deformation

• Downstream AO

Assumptions

• Most systems don’t interact• Separated physically and in bandwidth• Final image corrected by AO• Each previous system used to offload mean

positions.– E.g., M2 offloads AO to ~5 Hz– M1 fine offloads M2 to ~1 Hz– M1 gross offloads M1 fine to ~0.001 Hz

Assumptions (cont.)

• Separability of systems has limits– Motion of slow systems may induce vibrations– Some systems are partially redundant, so must

‘agree’ on how to remove certain errors (e.g., pointing)

• Some systems can’t avoid interaction– M2 fast positioner

Assumptions (cont.)

• Input must allow hierarchical approach

• Roll-off of errors must allow separation of high-bandwidth control from large structures.

• Wind is a key unknown– Magnitude of errors– Frequency content

Wind Data

• Gemini South 8m (Optical)– Structural (modal and operating)– Pressure on primary– Wind speed (on structure and dome)

• Nobeyama 45m (mm-Wave) – On-sky pointing– Structural (operating)– Controller

Gemini Data

• First round data (CD produced)– Modal Test– Operating Data– Wind pressures– DOE results

• Second round data (analysis beginning)– Wind speed and pressure only– Better coverage of parameter space

Nobeyama Data

• Goal was to investigate pointing– Pointing data analyzed– Structural data quick-look only

• Deformations relevant to GSMT– Similar size– Similar natural frequencies

Wind Effects

• Generally assumed to be low frequency– For 10m/s wind at 10m height

• Davenport Spectrum peaks at ~0.01 Hz• Antoniou spectrum peaks at ~0.1 Hz

• Roll-off is slow– Slope of -2/3 in typical approach to plotting

• Vortex generation from structure• All frequencies are affected

Wind Effects (cont.)

• All structural frequencies excited

• Amplitude drops as 1/²

• If a specific mode isn’t driven by a vortex, then deformations are unimportant above some frequency.

Nobeyama Results

• Deformation of the primary– Motion normal to surface– Rigid body tilt removed

• Motion of the secondary– X,Y,Z of typical point

Conditions of Tests

• Parked, calm (<2 m/s wind)– Benchmark case

• Tracking, calm– Effects of controller and motion

• Parked, windy (6-8 m/s)– Effects of wind

• No data tracking in wind

Deformations of the Primary

• Raw acceleration signal

• Removal of rigid body tilt

• Comparison of RMS deformation at/above a given frequency

Parked Telescope, Calm Wind

Tracking Telescope, Calm Wind

Parked Telescope, Wind 6-8m/s

RMS Comparison

Implications: Primary

• Total RMS error can be 10’s of microns

• Tracking is as important as wind– Hydrostatic bearings– Motion planning essential

• After ~3-4 Hz, residual is <1 m– Control of M1 would interact with structure– Low spatial frequency errors: M2 correction

Motion of the Secondary

• Accelerations in X, Y, Z

• RMS comparisons at/above a given frequency (X, Y, Z)

Parked Telescope, Calm Wind

Tracking Telescope, Calm Wind

Parked Telescope, Wind 6-8m/s

RMS Comparison, X

RMS Comparison, Y

RMS Comparison, Z

Implications: Secondary

• Twist motions much smaller• Tracking and wind cause same scale errors• Lateral and focus/tilt motions: 10’s of m• Most effects (>1m) below 3 Hz• M2 probably must correct ~3Hz effects

– Deformation– Position/tilt– Implies interaction with structure

Conclusions

• Data indicate likely size of errors

• Frequency range includes structural modes

• Seems to support hierarchical approach

• Interaction problem at M2

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