Attitude Determination and Control System Design for STU-2A Cubesat and In-Orbit Results

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13 th Annual Summer CubeSat Developer s Workshop August 6-7, 2016, Logan, Utah Attitude Determination and Control System Design for STU-2A Cubesat and In-Orbit Results Presented by Shufan Wu Guowen Sun, Xiwang Xia, Shufan Wu, Ziyi Wu, Wen Chen, Zhao Li Shanghai Engineering Centre for Microsatellites, Chinese Academy of Science, Shanghai, China shufan.wu@mail.sim.ac.cn

STU-2A Mission Overview Outline ADCS Hardware ADCS Algorithm In-orbit Data Analysis and Experiment Results Lessons learned

STU-2A Mission Overview 3U Cubesat with a mass of 2.9kg; 114 mm 114 mm 343.3 mm; Launched on Sept. 25, 2015. taking pictures of polar with an onboard CMOS color camera; Demonstration of Cubesats Networking based on Gamalink and CSP; Demonstration of MEMS based cold-gas micropropulsion ; In-orbit demonstration and verification of the GPS/Beidou receiver. STU-2 are the first batch of nano satellites in China that are made in accordance with the Cubesat standard.

STU-2A Mission Overview Satellite configuration STU-2A STU-2A BUS Payload MS&TCS CDHS ADCS EPS COM STX Structure On Board Computer Magnetometer Power Controler VHF/UHF Transceiver S-band Transmitter Camera Bumper P-POD Electric Heater Interface and Control System Corse Sun Sensor Fine Sun Sensor Rate Gyro Star Tracker 18650 Lithiumion Batteries Solar Cell VHF/UHF Antenna S-band Patch Antenna Gamslink Micropropulsion GPS/BeiDou receiver Multilayer Insulation Magnetorquer Thermal Control Coating Reaction Wheel

Requirements for ADCS STU-2A Mission Overview Vg t+s t h 0.6 GSD Pointing accuracy 2 Attitude stability 0.28 /s. Designed performance of ADCS ADCS Performance Value Attitude Determination Precision 1 (3σ) Pointing Accuracy 2 (3σ) Attitude Stabilization Precision 0.1 /s

ADCS Subsystem Architecture STU-2A Mission Overview Magnetometer x1 HMC5843 Fine Sun Sensor x1 FSS-4 I2C OBC PWM H-Bridge Magnetorquer X Magnetorquer Y Coarse Sun Sensor x5 Photodiode A/D Magnetorquer Z Sensors Command and Data Handling Actuators Rate Gyro x1 MPU-3300 Magnetometer x1 HMC5883L I2C HUB SPI Wheel Drive Electronic circuitry Reaction Wheel X RW-1 Reaction Wheel Y RW-1 Star Tracker x1 ST-200 UART Reaction Wheel Z RW-1

ADCS Hardware Sensors and Actuators Type Attitude Determination Sensors 3-Axis Magnetometer HMC5843 1 3-Axis Magnetometer HMC5883L 1 Coarse Sun Sensors SLCD-61N8 Photodiodes 5 MEMS 3-Axis gyro MPU-3300 1 Fine Sun Sensor FSS-4 1 Star Tracker ST-200 1 Attitude Control Actuators Magnetic coils 3 Reaction wheels RW-1 3

ADCS Algorithm Launch The basic algorithm is TRIAD, which determines the attitude by use of the knowledge from two non-parallel measuring vectors. Separated from Rocket Detumbling Idle Mode A UKF algorithm is combined into the TRIAD algorithm to improve the attitude accuracy. Sun Pointing Magnetic Control Momentum Biased Control Three Reaction Wheels Control

Detumbling Phase In-orbit Data Analysis and Results 94 minutes after launch, the first received signals showed that the satellite had completed rate damping (three axis angular velocity have been reduce within 0.3º/s) within one orbit period time and entered Sun Pointing Mode automatically. The in-orbit result was in conformity with simulation.

Sun Pointing / Sun Acquisition In-orbit Data Analysis and Results Sun vector in body coordinate system Charge-discharge curve (mv) The charge and discharge curve of STU-2A Charge cutoff voltage Discharge during eclipse Charge during light time

Nadir Pointing Mode In-orbit Data Analysis and Results Three attitude angles were constrained within 1º. The time period is from 08:20 to 08:26, 30 th Sep, 2015.

CMOS Camera Image In-orbit Data Analysis and Results Image of polar glaciers captured on Feb 23 00:10:30 2016 UTC Image of polar glaciers captured on Feb 23 23:41:34 2016 UTC

In-orbit Test Experiences Thruster Firing Micro-Propulsion In-Orbit Firing On Nov 5 th 2015, 10:09(UTC), thruster B and C are commanded for 5 min firing @ 1mN, aiming to raise the orbit Firing Results Thruster B falls into problem rapidly Unbalanced thrust level leads high rate spinning Spinning rate upto ca 65 deg/s (measured by redundant MEMS gyro on Nano-Hub) The resulted orbit change becomes very limited ca 0.6km 13

In-orbit Test Experiences Oscillation Local Oscillation work-point at ca 65 deg/s Initial tests try to reduce spin rate by counter-firing the thrusters Reduced 5 deg/s by firing in one pass, resumed back at ca 65 deg/s in next pass Reduced 10 deg/s by firing in one pass, back to 65 deg/s again in next pass Local Oscillation work-point at ca 65 deg/s Ts= 1 sec delay in the magnetic control loop (take the measurement before sending out the magnetic control, to separate disturbance) This delay in the control loop results in a steady oscillation work-point Simulation results revealed the oscillation work-point at ca 65 deg/s If remove the delay in simulation, the oscillation disappear Condition back to 0 work-point Simulation shows, the initial rate needs to be below 20 deg/s Then, magnetic control can reduce the rate down to zero 14

Rescue Process Switch off ADCS loop 7 days successive firing to reduce the rate Rate down to ca 14 deg/s Switch on the ADCS Magnetic control bring the spin rate down to zero Thanks to: In-orbit Test Experiences Attitude Rescue Successful l Rescue around the 2015 Xmas week CSP allows direct access to subsystem redundant MEMS gyro and magnetometer Open-loop control Sequence of thrust firings to de-spin the STU-2A 15

Problems and Lessons Learned (1) Redundant back ups of key sensors & actuators Redundant MEMS gyro Redundant magnetometer Cold-gas thrusters - additional measure for attitude Magnetic residuals leads to rotation in pitch axis one rotation / orbit accurate attitude performance was not achieved in STU-2A the 18650 lithium-ion batteries could pose magnetic dipole In-orbit injection of control parameters & software patches very important to calibrate off-set or errors if so, residual dipole can be compensated if so, oscillation work-point @ 65deg/s can be removed 16

Magnetic Rod vs Magnetic Coil Magnetometer & Magnetorque layout Sensors testing coverage Problems and Lessons Learned (2) Magnetic rod gives higher flux than coils built in the PCB Thus to have more capacity to fight magnetic residuas Rod is preferred if space allows Magnetometer shall be kept away from large current devices, e.g. PC-104 socket (TM pulses cause high current, ) Magnetomer far away from magnetic coils or rods if possible Mangetometer on a deployed boom is preferred if possible Fine sun sensor testing was not professional, accuracy degraded Shall use Sun simulator at varying angles and temperatures to calibrate the accuracy 17

18 Prof Dr Shufan Wu Chinese Academy of Science(CAS) Shanghai Engineering Centre for Microsatellite Emial: shufan.wu@mail.sim.ac.cn Tel:021-50735022,15800537342