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Published byDomenic Caldwell Modified over 9 years ago
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George Angeli 11 September, 2001 Current Concepts and Status of GSMT Control Systems
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Introduction l Feasibility of GSMT depends on its controllability Segment alignment maintenance Wind effect compensation (structure correction) l Whatever is designed, it must be observable and CONTROLLABLE! l How does the boot get on the dinner table? Why do we care about the control system in this early phase of design?
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Frequency Band Separation of Subsystems 0.0010.010.1110100 Bandwidth [Hz] Zernike modes ~100 ~50 ~20 ~10 2 aO (M1) AO (M2) Main Axes LGS MCAO Secondary rigid body temporal avg spatial & temporal avg spatial avg
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MCAO l MCAO can be separated from telescope control First MCAO sensor is behind the last telescope control actuator in the light path MCAO is fed with a wavefront corrected up to 30-50 Zernike @ 20 Hz BW on tracking guide star
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Active Optics l Initial phasing in open loop Low spatial frequencies barely observable by edge sensors l Phasing maintenance in closed loop with edge sensors Assumption: wind buffeting has negligible high spatial frequency effects on primary mirror Continuity maintenance system is static (no interference with structural resonances)
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Phasing Maintenance l Static influence function l Edge detector / actuator modes by SVD
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Control Configuration for Phasing Maintenance From phasing Edge sensors Actuator space Pseudo-inverse:
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Adaptive Optics l Adaptive (deformable) secondary Atmospheric correction r 0 0.5 m @ 1.2 ~7000 actuators for 30 m MMT 1200 actuator/m 2 on secondary@ 0.6 m GSMT 2200 actuator/m 2 on secondary@ 2 m Telescope deformation correction max. 1800 actuators for 600 segments 570 actuators/m 2 on secondary In the close future atmospheric correction is not feasible in the NIR (maybe in midIR)
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Deformable Secondary l Face-sheet mass is negligible No interaction with telescope structure l Face-sheet motion is over-damped No local dynamics Secondary AO system is static l Wavefront correction with deformable secondary Temporal average (0.1 Hz) off-loaded on primary
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Frequency Band Separation of Wavefront Correction and Tracking
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Control Configuration for Wavefront Correction and Tracking Measurement noiseWind, Gravity, HeatAtmosphere Offset due to: telescope aberration off-axis guide star
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Physical Configuration
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Computational Load l Static active optics l Deformable secondary 1 Hz bandwidth 10 Hz sampling rate Reconstructor matrix [1800 x 3600] 2 sensors on each edge 230 GFLOP/s 20 Hz bandwidth 200 Hz sampling rate Reconstructor matrix [1800 x 1000] 360 GFLOP/s Texas TMS320C64x 4.8 GFLOP/s Intel P4 1.4GHz 5.6 GFLOP/s
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System Modeling and Simulation l Investigate telescope behavior l Validate design assumptions Observability (sensor choices, placement) Controllability (actuator choices, placement) l Allows modal-based feedback design (Linear Quadratic Gaussian, H , etc.) Performance l Validate model reduction for simulation and control
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Current Model l Modal based state space representation of the structure, based on FEA (20 modes) Primary mirror as a surface fit on raft support nodes Line-of-sight equation for rigid body motion of primary and secondary Force actuators at weakened or completely opened degrees of freedom l Zernike representation of wavefront quality l Integrated structure FEA Redefined base for OPD as a linear combination of Zernikes linked to structural modes
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Primary Mirror Truss Structure
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Structural Mode Shapes on the Primary Mirror
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Zernike Content of the Structural Modes
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Zernike Content of Secondary Rigid Body Motion
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Wind Load (X Direction)
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Wind Load (Y Direction)
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Wind Load (Z Direction)
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Future Path l Wavefront control (wind buffeting) Segmented primary model (edge detectors, detector and actuator mode spaces) Verification of ‘static phasing maintenance’ hypothesis l Primary control Feedback design and simulation Deformable secondary ‘surface fit’ model Primary ‘surface fit’ model on actuator nodes Wind load definition (on structure and primary) Feedback design and simulation
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Future Path (cont’d) l Tracking Actuator definition Nonlinear (large signal) and linearized (small signal) models Gravitational load definition Feedback design and simulation l Integration Structural model integration Optical model integration Feedback integration and simulation
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Modeling Issues l Structural model Integrated structure versus interfaced subsystems Boundary value problems l Optical model Refined ‘fitted surface’ model with ray tracing and fitting each structural modes, i.e. building a new orthogonal basis for OPD which is characteristic to the telescope Segmented mirror optical response l Load model Wind power spectral density and spatial distribution Wind-to-force conversion
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