FAULT DETECTION for SPACECRAFT ATTITUDE CONTROL SYSTEM. M. Amin Vahid D. Mechanical Engineering Department Concordia University December 19 th, 2010

Size: px
Start display at page:

Download "FAULT DETECTION for SPACECRAFT ATTITUDE CONTROL SYSTEM. M. Amin Vahid D. Mechanical Engineering Department Concordia University December 19 th, 2010"

Transcription

1 FAULT DETECTION for SPACECRAFT ATTITUDE CONTROL SYSTEM M. Amin Vahid D. Mechanical Engineering Department Concordia University December 19 th, 2010

2 Attitude control : the exercise of control over the orientation of an object with respect to an inertial frame of reference or another entity (the celestial sphere, certain fields, nearby objects, etc.).

3 Controlling vehicle attitude requires : sensors to measure vehicle attitude actuators to apply the torques needed to re-orient the vehicle to a desired attitude algorithms to command the actuators based on (1) sensor measurements of the current attitude and (2) specification of a desired attitude.

4 Momentum wheels These are electric motor driven rotors made to spin in the direction opposite to that required to re-orient the vehicle. Since momentum wheels make up a small fraction of the spacecraft's mass and are computer controlled, they give precise control.

5 Momentum wheels are generally suspended on magnetic bearings to avoid bearing friction and breakdown problems. To maintain orientation in three dimensional space a minimum of two must be used, with additional units providing single failure protection.

6 Spacecraft systems need increased on board autonomy to detect the occurred faults, isolate the faulty components, and effectively handle their operation in the presence of such faults. In this research a scheme of fault detection and diagnosis is developed for spacecraft Attitude Control System.

7 Fault detection and isolation a subfield of control engineering which concerns itself with monitoring a system, identifying when a fault has occurred, and pinpointing the type of fault and its location.

8 Fault detection: the identification of the presence of an unknown fault.

9 FDD Methods Analythical Redundancy Hrdware Redundancy Model Base Signal Base Heuristic Model Analytical Model Spectrum Analysis Wavelet Techniques Expert Knowledge Base/Neural Network System State EStimation Parameter estimation

10 Model-based FDI In model-based FDI techniques some model of the system is used to decide about the occurrence of fault. The system model may be mathematical, or knowledge based. Some of the model-based FDI techniques include observer-based approach, parityspace approach, and parameter identification based methods.

11 State estimation approach In the Kalman Filter method, the innovation of K.F is used as the fault detection residual. This residual is white and has a zero mean under nonfaulty conditions, and becomes non-zero in the presence of a fault. The key idea in the parity relation approach is to check the consistency of the mathematical equations of the system (analytical redundancy relations) by using the actual measurements. In this method, residuals are colored and disturbance decoupling improves.

12 Description and Modeling of Spacecraft Attitude Control System Equations of motion:

13 In the other hand so :

14 Reference frame

15 ω RIB C θ C ψ C θ S ψ S θ S ψ C φ S φ S θ C ψ C ψ C φ S φ S θ S ψ S φ C θ S φ S ψ C φ S θ C ψ S φ C ψ C φ S θ S ψ C φ C θ 0 ω 0 0 ω BR M I S h w ω BI h B h w I S I S ω RIB p q r Q ϕ θ ψ

16 M G Reaction wheels we have: w w dem Max angular moment 0.2Nm/s Max angular velacity 280 rad/sec Inertia moment Nominal Velocity Nominal torque kgm2 100 rad/sec 1 N.m

17 Linearization

18

19 Computing the state transition matrix

20 The linear state space representation of the process model: The covariance matrix M before the:

21 Computing the Kalman gain matrix K Kalman Filter as a Residual Generator

22

23

24

25

26 Euler angles (fault-free) Angular velocity (fault-free)

27 Euler angle (fault injected for in t=13s) Residuals (fault injected in t=13s)

28 Thank you Happy New Year!

29

AS3010: Introduction to Space Technology

AS3010: Introduction to Space Technology AS3010: Introduction to Space Technology L E C T U R E 22 Part B, Lecture 22 19 April, 2017 C O N T E N T S Attitude stabilization passive and active. Actuators for three axis or active stabilization.

More information

Application of Adaptive Thresholds in Robust Fault Detection of an Electro- Mechanical Single-Wheel Steering Actuator

Application of Adaptive Thresholds in Robust Fault Detection of an Electro- Mechanical Single-Wheel Steering Actuator Preprints of the 8th IFAC Symposium on Fault Detection, Supervision and Safety of Technical Processes (SAFEPROCESS) August 29-31, 212. Mexico City, Mexico Application of Adaptive Thresholds in Robust Fault

More information

Sliding Mode Control Strategies for Spacecraft Rendezvous Maneuvers

Sliding Mode Control Strategies for Spacecraft Rendezvous Maneuvers Osaka University March 15, 2018 Sliding Mode Control Strategies for Spacecraft Rendezvous Maneuvers Elisabetta Punta CNR-IEIIT, Italy Problem Statement First Case Spacecraft Model Position Dynamics Attitude

More information

Spacecraft Attitude Control using CMGs: Singularities and Global Controllability

Spacecraft Attitude Control using CMGs: Singularities and Global Controllability 1 / 28 Spacecraft Attitude Control using CMGs: Singularities and Global Controllability Sanjay Bhat TCS Innovation Labs Hyderabad International Workshop on Perspectives in Dynamical Systems and Control

More information

MAE 142 Homework #5 Due Friday, March 13, 2009

MAE 142 Homework #5 Due Friday, March 13, 2009 MAE 142 Homework #5 Due Friday, March 13, 2009 Please read through the entire homework set before beginning. Also, please label clearly your answers and summarize your findings as concisely as possible.

More information

A Multiple-Observer Scheme for Fault Detection, Isolation and Recovery of Satellite Thrusters

A Multiple-Observer Scheme for Fault Detection, Isolation and Recovery of Satellite Thrusters Proceedings of the EuroGNC 3, nd CEAS Specialist Conference on Guidance, Navigation & Control, Delft University of Technology, Delft, The Netherlands, April -, 3 FrBT.3 A Multiple-Observer Scheme for Fault

More information

An Attitude Control System and Commissioning Results of the SNAP-1 Nanosatellite

An Attitude Control System and Commissioning Results of the SNAP-1 Nanosatellite An Attitude Control System and Commissioning Results of the SNAP-1 Nanosatellite WH Steyn, Y Hashida and V Lappas Surrey Space Centre University of Surrey Guildford, Surrey GU2 5XH United Kingdom Abstract.

More information

THE REACTION WHEEL PENDULUM

THE REACTION WHEEL PENDULUM THE REACTION WHEEL PENDULUM By Ana Navarro Yu-Han Sun Final Report for ECE 486, Control Systems, Fall 2013 TA: Dan Soberal 16 December 2013 Thursday 3-6pm Contents 1. Introduction... 1 1.1 Sensors (Encoders)...

More information

Adaptive Unscented Kalman Filter with Multiple Fading Factors for Pico Satellite Attitude Estimation

Adaptive Unscented Kalman Filter with Multiple Fading Factors for Pico Satellite Attitude Estimation Adaptive Unscented Kalman Filter with Multiple Fading Factors for Pico Satellite Attitude Estimation Halil Ersin Söken and Chingiz Hajiyev Aeronautics and Astronautics Faculty Istanbul Technical University

More information

Active Diagnosis of Hybrid Systems Guided by Diagnosability Properties

Active Diagnosis of Hybrid Systems Guided by Diagnosability Properties Active Diagnosis of Hybrid Systems Guided by Diagnosability Properties Application to autonomous satellites Louise Travé-Massuyès 5 February 29 Motivation Control and autonomy of complex dynamic systems

More information

Supervisor: Dr. Youmin Zhang Amin Salar Zahra Gallehdari Narges Roofigari

Supervisor: Dr. Youmin Zhang Amin Salar Zahra Gallehdari Narges Roofigari Supervisor: Dr. Youmin Zhang Amin Salar 6032761 Zahra Gallehdari 1309102 Narges Roofigari 8907926 Fault Diagnosis and Fault Tolerant Control Systems Final Project December 2011 Contents Introduction Quad-Rotor

More information

Lecture Module 5: Introduction to Attitude Stabilization and Control

Lecture Module 5: Introduction to Attitude Stabilization and Control 1 Lecture Module 5: Introduction to Attitude Stabilization and Control Lectures 1-3 Stability is referred to as a system s behaviour to external/internal disturbances (small) in/from equilibrium states.

More information

Attitude Determination and. Attitude Control

Attitude Determination and. Attitude Control Attitude Determination and Placing the telescope in orbit is not the end of the story. It is necessary to point the telescope towards the selected targets, or to scan the selected sky area with the telescope.

More information

IROS 16 Workshop: The Mechatronics behind Force/Torque Controlled Robot Actuation Secrets & Challenges

IROS 16 Workshop: The Mechatronics behind Force/Torque Controlled Robot Actuation Secrets & Challenges Arne Wahrburg (*), 2016-10-14 Cartesian Contact Force and Torque Estimation for Redundant Manipulators IROS 16 Workshop: The Mechatronics behind Force/Torque Controlled Robot Actuation Secrets & Challenges

More information

Analytical Disturbance Modeling of a Flywheel Due to Statically and Dynamically Unbalances

Analytical Disturbance Modeling of a Flywheel Due to Statically and Dynamically Unbalances Journal of mathematics and computer Science 9 (2014) 139-148 Analytical Disturbance Modeling of a Flywheel Due to Statically and Dynamically Unbalances Amir Karimian 1, Saied Shokrollahi 2, Shahram Yousefi

More information

A Neural Network Approach to Fault Detection in Spacecraft Attitude Determination and Control Systems

A Neural Network Approach to Fault Detection in Spacecraft Attitude Determination and Control Systems Utah State University DigitalCommons@USU All Graduate Theses and Dissertations Graduate Studies 5-2015 A Neural Network Approach to Fault Detection in Spacecraft Attitude Determination and Control Systems

More information

Quaternion-Based Tracking Control Law Design For Tracking Mode

Quaternion-Based Tracking Control Law Design For Tracking Mode A. M. Elbeltagy Egyptian Armed forces Conference on small satellites. 2016 Logan, Utah, USA Paper objectives Introduction Presentation Agenda Spacecraft combined nonlinear model Proposed RW nonlinear attitude

More information

Mechatronics Assignment # 1

Mechatronics Assignment # 1 Problem # 1 Consider a closed-loop, rotary, speed-control system with a proportional controller K p, as shown below. The inertia of the rotor is J. The damping coefficient B in mechanical systems is usually

More information

Satellite Attitude Control System Design Using Reaction Wheels Bhanu Gouda Brian Fast Dan Simon

Satellite Attitude Control System Design Using Reaction Wheels Bhanu Gouda Brian Fast Dan Simon Satellite Attitude Control System Design Using Reaction Wheels Bhanu Gouda Brian Fast Dan Simon Outline 1. Overview of Attitude Determination and Control system. Problem formulation 3. Control schemes

More information

Wind Turbine Fault Detection Using Counter-Based Residual Thresholding

Wind Turbine Fault Detection Using Counter-Based Residual Thresholding Wind Turbine Fault Detection Using Counter-Based Residual Thresholding Ahmet Arda Ozdemir, Peter Seiler, and Gary J. Balas Department of Aerospace Engineering and Mechanics, University of Minnesota, Minneapolis,

More information

AIRCRAFT BRAKING DYNAMICS AND BRAKE SYSTEM MODELING FOR FAULT DETECTION AND ISOLATION

AIRCRAFT BRAKING DYNAMICS AND BRAKE SYSTEM MODELING FOR FAULT DETECTION AND ISOLATION AIRCRAFT BRAKING DYNAMICS AND BRAKE SYSTEM MODELING FOR FAULT DETECTION AND ISOLATION Lucas Cardoso Navarro ITA São José dos Campos, São Paulo, Brazil Luiz Carlos Sandoval Goes ITA São José dos Campos,

More information

EXAMPLE: MODELING THE PT326 PROCESS TRAINER

EXAMPLE: MODELING THE PT326 PROCESS TRAINER CHAPTER 1 By Radu Muresan University of Guelph Page 1 EXAMPLE: MODELING THE PT326 PROCESS TRAINER The PT326 apparatus models common industrial situations in which temperature control is required in the

More information

CS491/691: Introduction to Aerial Robotics

CS491/691: Introduction to Aerial Robotics CS491/691: Introduction to Aerial Robotics Topic: Midterm Preparation Dr. Kostas Alexis (CSE) Areas of Focus Coordinate system transformations (CST) MAV Dynamics (MAVD) Navigation Sensors (NS) State Estimation

More information

Handling parametric and non-parametric additive faults in LTV Systems

Handling parametric and non-parametric additive faults in LTV Systems 1 / 16 Handling parametric and non-parametric additive faults in LTV Systems Qinghua Zhang & Michèle Basseville INRIA & CNRS-IRISA, Rennes, France 9th IFAC SAFEPROCESS, Paris, France, Sept. 2-4, 2015 2

More information

3 Rigid Spacecraft Attitude Control

3 Rigid Spacecraft Attitude Control 1 3 Rigid Spacecraft Attitude Control Consider a rigid spacecraft with body-fixed frame F b with origin O at the mass centre. Let ω denote the angular velocity of F b with respect to an inertial frame

More information

A Physically-Based Fault Detection and Isolation Method and Its Uses in Robot Manipulators

A Physically-Based Fault Detection and Isolation Method and Its Uses in Robot Manipulators des FA 4.13 Steuerung und Regelung von Robotern A Physically-Based Fault Detection and Isolation Method and Its Uses in Robot Manipulators Alessandro De Luca Dipartimento di Informatica e Sistemistica

More information

TTK4190 Guidance and Control Exam Suggested Solution Spring 2011

TTK4190 Guidance and Control Exam Suggested Solution Spring 2011 TTK4190 Guidance and Control Exam Suggested Solution Spring 011 Problem 1 A) The weight and buoyancy of the vehicle can be found as follows: W = mg = 15 9.81 = 16.3 N (1) B = 106 4 ( ) 0.6 3 3 π 9.81 =

More information

A New Model Reference Adaptive Formulation to Estimate Stator Resistance in Field Oriented Induction Motor Drive

A New Model Reference Adaptive Formulation to Estimate Stator Resistance in Field Oriented Induction Motor Drive A New Model Reference Adaptive Formulation to Estimate Stator Resistance in Field Oriented Induction Motor Drive Saptarshi Basak 1, Chandan Chakraborty 1, Senior Member IEEE and Yoichi Hori 2, Fellow IEEE

More information

Simplified Filtering Estimator for Spacecraft Attitude Determination from Phase Information of GPS Signals

Simplified Filtering Estimator for Spacecraft Attitude Determination from Phase Information of GPS Signals WCE 7, July - 4, 7, London, U.K. Simplified Filtering Estimator for Spacecraft Attitude Determination from Phase Information of GPS Signals S. Purivigraipong, Y. Hashida, and M. Unwin Abstract his paper

More information

Sensors for mobile robots

Sensors for mobile robots ROBOTICS 01PEEQW Basilio Bona DAUIN Politecnico di Torino Mobile & Service Robotics Sensors for Robotics 2 Sensors for mobile robots Sensors are used to perceive, analyze and understand the environment

More information

Lab #4 - Gyroscopic Motion of a Rigid Body

Lab #4 - Gyroscopic Motion of a Rigid Body Lab #4 - Gyroscopic Motion of a Rigid Body Last Updated: April 6, 2007 INTRODUCTION Gyroscope is a word used to describe a rigid body, usually with symmetry about an axis, that has a comparatively large

More information

Fault-Tolerant Control Strategies for a Class of Euler-Lagrange Nonlinear Systems Subject to Simultaneous Sensor and Actuator Faults

Fault-Tolerant Control Strategies for a Class of Euler-Lagrange Nonlinear Systems Subject to Simultaneous Sensor and Actuator Faults Fault-Tolerant Control Strategies for a Class of Euler-Lagrange Nonlinear Systems Subject to Simultaneous Sensor and Actuator Faults Maryam Abdollahi A Thesis in The Department of Electrical and Computer

More information

Exercise 5 - Hydraulic Turbines and Electromagnetic Systems

Exercise 5 - Hydraulic Turbines and Electromagnetic Systems Exercise 5 - Hydraulic Turbines and Electromagnetic Systems 5.1 Hydraulic Turbines Whole courses are dedicated to the analysis of gas turbines. For the aim of modeling hydraulic systems, we analyze here

More information

Sensorless Control for High-Speed BLDC Motors With Low Inductance and Nonideal Back EMF

Sensorless Control for High-Speed BLDC Motors With Low Inductance and Nonideal Back EMF Sensorless Control for High-Speed BLDC Motors With Low Inductance and Nonideal Back EMF P.Suganya Assistant Professor, Department of EEE, Bharathiyar Institute of Engineering for Women Salem (DT). Abstract

More information

Jitter and Basic Requirements of the Reaction Wheel Assembly in the Attitude Control System

Jitter and Basic Requirements of the Reaction Wheel Assembly in the Attitude Control System Jitter and Basic Requirements of the Reaction Wheel Assembly in the Attitude Control System Lulu Liu August, 7 1 Brief Introduction Photometric precision is a major concern in this space mission. A pointing

More information

Chapters 10 & 11: Rotational Dynamics Thursday March 8 th

Chapters 10 & 11: Rotational Dynamics Thursday March 8 th Chapters 10 & 11: Rotational Dynamics Thursday March 8 th Review of rotational kinematics equations Review and more on rotational inertia Rolling motion as rotation and translation Rotational kinetic energy

More information

DC Motor Position: System Modeling

DC Motor Position: System Modeling 1 of 7 01/03/2014 22:07 Tips Effects TIPS ABOUT BASICS INDEX NEXT INTRODUCTION CRUISE CONTROL MOTOR SPEED MOTOR POSITION SUSPENSION INVERTED PENDULUM SYSTEM MODELING ANALYSIS DC Motor Position: System

More information

Predictive Control of Gyroscopic-Force Actuators for Mechanical Vibration Damping

Predictive Control of Gyroscopic-Force Actuators for Mechanical Vibration Damping ARC Centre of Excellence for Complex Dynamic Systems and Control, pp 1 15 Predictive Control of Gyroscopic-Force Actuators for Mechanical Vibration Damping Tristan Perez 1, 2 Joris B Termaat 3 1 School

More information

Neural Networks Lecture 10: Fault Detection and Isolation (FDI) Using Neural Networks

Neural Networks Lecture 10: Fault Detection and Isolation (FDI) Using Neural Networks Neural Networks Lecture 10: Fault Detection and Isolation (FDI) Using Neural Networks H.A. Talebi Farzaneh Abdollahi Department of Electrical Engineering Amirkabir University of Technology Winter 2011.

More information

Teacher s notes 35 Conservation of angular momentum (1)

Teacher s notes 35 Conservation of angular momentum (1) Sensors: Loggers: Rotary Motion Any EASYSENSE Physics Logging time: 10 seconds Teacher s notes 35 Conservation of angular momentum (1) Introduction The use of the disc accessories allows the Rotary Motion

More information

Passive Magnetic Attitude Control for CubeSat Spacecraft

Passive Magnetic Attitude Control for CubeSat Spacecraft Passive Magnetic Attitude Control for CubeSat Spacecraft David Gerhardt Advisor: Dr. Scott Palo University of Colorado at Boulder Department of Aerospace Engineering Sciences August 11, 2010 Motivation

More information

Generation X. Attitude Control Systems (ACS) Aprille Ericsson Dave Olney Josephine San. July 27, 2000

Generation X. Attitude Control Systems (ACS) Aprille Ericsson Dave Olney Josephine San. July 27, 2000 Generation X Attitude Control Systems (ACS) Aprille Ericsson Dave Olney Josephine San July 27, 2000 ACS Overview Requirements Assumptions Disturbance Torque Assessment Component and Control Mode Recommendations

More information

A Ferris wheel in Japan has a radius of 50m and a mass of 1.2 x 10 6 kg. If a torque of 1 x 10 9 Nm is needed to turn the wheel when it starts at

A Ferris wheel in Japan has a radius of 50m and a mass of 1.2 x 10 6 kg. If a torque of 1 x 10 9 Nm is needed to turn the wheel when it starts at Option B Quiz 1. A Ferris wheel in Japan has a radius of 50m and a mass of 1. x 10 6 kg. If a torque of 1 x 10 9 Nm is needed to turn the wheel when it starts at rest, what is the wheel s angular acceleration?

More information

1. The first thing you need to find is the mass of piece three. In order to find it you need to realize that the masses of the three pieces must be

1. The first thing you need to find is the mass of piece three. In order to find it you need to realize that the masses of the three pieces must be 1. The first thing you need to find is the mass of piece three. In order to find it you need to realize that the masses of the three pieces must be equal to the initial mass of the starting rocket. Now

More information

Visual Feedback Attitude Control of a Bias Momentum Micro Satellite using Two Wheels

Visual Feedback Attitude Control of a Bias Momentum Micro Satellite using Two Wheels Visual Feedback Attitude Control of a Bias Momentum Micro Satellite using Two Wheels Fuyuto Terui a, Nobutada Sako b, Keisuke Yoshihara c, Toru Yamamoto c, Shinichi Nakasuka b a National Aerospace Laboratory

More information

Design and performance simulation of a satellite momentum exchange actuator

Design and performance simulation of a satellite momentum exchange actuator Australian Journal of Mechanical Engineering ISSN: 1448-4846 (Print) 2204-2253 (Online) Journal homepage: http://www.tandfonline.com/loi/tmec20 Design and performance simulation of a satellite momentum

More information

Rigid bodies - general theory

Rigid bodies - general theory Rigid bodies - general theory Kinetic Energy: based on FW-26 Consider a system on N particles with all their relative separations fixed: it has 3 translational and 3 rotational degrees of freedom. Motion

More information

Chapter 11 Angular Momentum; General Rotation. Copyright 2009 Pearson Education, Inc.

Chapter 11 Angular Momentum; General Rotation. Copyright 2009 Pearson Education, Inc. Chapter 11 Angular Momentum; General Rotation ! L = I!! Units of Chapter 11 Angular Momentum Objects Rotating About a Fixed Axis Vector Cross Product; Torque as a Vector Angular Momentum of a Particle

More information

Spinning Satellites Examples. ACS: Gravity Gradient. ACS: Single Spin

Spinning Satellites Examples. ACS: Gravity Gradient. ACS: Single Spin Attitude Determination and Attitude Control Placing the telescope in orbit is not the end of the story. It is necessary to point the telescope towards the selected targets, or to scan the selected sky

More information

General Definition of Torque, final. Lever Arm. General Definition of Torque 7/29/2010. Units of Chapter 10

General Definition of Torque, final. Lever Arm. General Definition of Torque 7/29/2010. Units of Chapter 10 Units of Chapter 10 Determining Moments of Inertia Rotational Kinetic Energy Rotational Plus Translational Motion; Rolling Why Does a Rolling Sphere Slow Down? General Definition of Torque, final Taking

More information

Satellite Attitude Determination with Attitude Sensors and Gyros using Steady-state Kalman Filter

Satellite Attitude Determination with Attitude Sensors and Gyros using Steady-state Kalman Filter Satellite Attitude Determination with Attitude Sensors and Gyros using Steady-state Kalman Filter Vaibhav V. Unhelkar, Hari B. Hablani Student, email: v.unhelkar@iitb.ac.in. Professor, email: hbhablani@aero.iitb.ac.in

More information

Design of Attitude Determination and Control Subsystem

Design of Attitude Determination and Control Subsystem Design of Attitude Determination and Control Subsystem 1) Control Modes and Requirements Control Modes: Control Modes Explanation 1 ) Spin-Up Mode - Acquisition of Stability through spin-up maneuver -

More information

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos Lecture 6: Modeling of Electromechanical Systems Principles of Motor Operation

More information

Rotational Motion, Torque, Angular Acceleration, and Moment of Inertia. 8.01t Nov 3, 2004

Rotational Motion, Torque, Angular Acceleration, and Moment of Inertia. 8.01t Nov 3, 2004 Rotational Motion, Torque, Angular Acceleration, and Moment of Inertia 8.01t Nov 3, 2004 Rotation and Translation of Rigid Body Motion of a thrown object Translational Motion of the Center of Mass Total

More information

COMPARISON OF FDI METHODS APPLIED ON NANOSATELLITES WITH ACTUATORS FAILURES

COMPARISON OF FDI METHODS APPLIED ON NANOSATELLITES WITH ACTUATORS FAILURES U.P.B. Sci. Bull., Seria D, Vol, 77, Iss 2, 2015 ISSN 1454-2358 COMPARISON OF FDI METHODS APPLIED ON NANOSATELLITES WITH ACTUATORS FAILURES Silvana RADU 1, Claudiu Ionuţ CHERCIU 2, Adrian-Mihail STOICA

More information

Spacecraft Attitude Control with RWs via LPV Control Theory: Comparison of Two Different Methods in One Framework

Spacecraft Attitude Control with RWs via LPV Control Theory: Comparison of Two Different Methods in One Framework Trans. JSASS Aerospace Tech. Japan Vol. 4, No. ists3, pp. Pd_5-Pd_, 6 Spacecraft Attitude Control with RWs via LPV Control Theory: Comparison of Two Different Methods in One Framework y Takahiro SASAKI,),

More information

Attitude Control Simulator for the Small Satellite and Its Validation by On-orbit Data of QSAT-EOS

Attitude Control Simulator for the Small Satellite and Its Validation by On-orbit Data of QSAT-EOS SSC17-P1-17 Attitude Control Simulator for the Small Satellite and Its Validation by On-orbit Data of QSAT-EOS Masayuki Katayama, Yuta Suzaki Mitsubishi Precision Company Limited 345 Kamikmachiya, Kamakura

More information

Mixed Control Moment Gyro and Momentum Wheel Attitude Control Strategies

Mixed Control Moment Gyro and Momentum Wheel Attitude Control Strategies AAS03-558 Mixed Control Moment Gyro and Momentum Wheel Attitude Control Strategies C. Eugene Skelton II and Christopher D. Hall Department of Aerospace & Ocean Engineering Virginia Polytechnic Institute

More information

Physics 180A Test Points

Physics 180A Test Points Physics 180A Test 3-10 Points Name You must complete six of the nine 10-point problems. You must completely cross off three 10-problems, thanks. Place your answers in the answer box. Watch your units and

More information

Phys 270 Final Exam. Figure 1: Question 1

Phys 270 Final Exam. Figure 1: Question 1 Phys 270 Final Exam Time limit: 120 minutes Each question worths 10 points. Constants: g = 9.8m/s 2, G = 6.67 10 11 Nm 2 kg 2. 1. (a) Figure 1 shows an object with moment of inertia I and mass m oscillating

More information

Fault Isolation of an Electro-mechanical Linear Actuator

Fault Isolation of an Electro-mechanical Linear Actuator Fault Isolation of an Electro-mechanical Linear Actuator Matt Kemp 1, and Eric J. Martin 2 1,2 Monterey Bay Aquarium Research Institute, Moss Landing, CA, 95039, USA mkemp@mbari.org emartin@mbari.org ABSTRACT

More information

FAULT DETECTION ON A REACTION WHEEL BASED ON PARAMETER ESTIMATION

FAULT DETECTION ON A REACTION WHEEL BASED ON PARAMETER ESTIMATION FAULT DETECTION ON A REACTION WHEEL BASED ON PARAMETER ESTIMATION Alexandre Carvalho Leite, Hélio Koiti Kuga, Roberto Vieira da Fonseca Lopes Av. dos Astronautas, 1.758, Jd. Granja, Ed. Satélite Av. dos

More information

Fault Diagnosis and Fault-Tolerant Control of Quadrotor UAVs

Fault Diagnosis and Fault-Tolerant Control of Quadrotor UAVs Wright State University CORE Scholar Browse all Theses and Dissertations Theses and Dissertations 2016 Fault Diagnosis and Fault-Tolerant Control of Quadrotor UAVs Remus C. Avram Wright State University

More information

Moment of Inertia Race

Moment of Inertia Race Review Two points, A and B, are on a disk that rotates with a uniform speed about an axis. Point A is closer to the axis than point B. Which of the following is NOT true? 1. Point B has the greater tangential

More information

Fault Detection and Isolation of the Wind Turbine Benchmark: an Estimation-based Approach

Fault Detection and Isolation of the Wind Turbine Benchmark: an Estimation-based Approach Milano (Italy) August - September, 11 Fault Detection and Isolation of the Wind Turbine Benchmark: an Estimation-based Approach Xiaodong Zhang, Qi Zhang Songling Zhao Riccardo Ferrari Marios M. Polycarpou,andThomas

More information

Dynamics. describe the relationship between the joint actuator torques and the motion of the structure important role for

Dynamics. describe the relationship between the joint actuator torques and the motion of the structure important role for Dynamics describe the relationship between the joint actuator torques and the motion of the structure important role for simulation of motion (test control strategies) analysis of manipulator structures

More information

Controllability Analysis of A Two Degree of Freedom Nonlinear Attitude Control System

Controllability Analysis of A Two Degree of Freedom Nonlinear Attitude Control System Controllability Analysis of A Two Degree of Freedom Nonlinear Attitude Control System Jinglai Shen, Amit K Sanyal, and N Harris McClamroch Department of Aerospace Engineering The University of Michigan

More information

ET3-7: Modelling I(V) Introduction and Objectives. Electrical, Mechanical and Thermal Systems

ET3-7: Modelling I(V) Introduction and Objectives. Electrical, Mechanical and Thermal Systems ET3-7: Modelling I(V) Introduction and Objectives Electrical, Mechanical and Thermal Systems Objectives analyse and model basic linear dynamic systems -Electrical -Mechanical -Thermal Recognise the analogies

More information

Model Based Fault Detection and Diagnosis Using Structured Residual Approach in a Multi-Input Multi-Output System

Model Based Fault Detection and Diagnosis Using Structured Residual Approach in a Multi-Input Multi-Output System SERBIAN JOURNAL OF ELECTRICAL ENGINEERING Vol. 4, No. 2, November 2007, 133-145 Model Based Fault Detection and Diagnosis Using Structured Residual Approach in a Multi-Input Multi-Output System A. Asokan

More information

CHAPTER 8 CONSERVATION LAWS

CHAPTER 8 CONSERVATION LAWS CHAPTER 8 CONSERVATION LAWS Outlines 1. Charge and Energy 2. The Poynting s Theorem 3. Momentum 4. Angular Momentum 2 Conservation of charge and energy The net amount of charges in a volume V is given

More information

Line following of a mobile robot

Line following of a mobile robot Line following of a mobile robot May 18, 004 1 In brief... The project is about controlling a differential steering mobile robot so that it follows a specified track. Steering is achieved by setting different

More information

Fault Detection and Diagnosis for a Three-tank system using Structured Residual Approach

Fault Detection and Diagnosis for a Three-tank system using Structured Residual Approach Fault Detection and Diagnosis for a Three-tank system using Structured Residual Approach A.Asokan and D.Sivakumar Department of Instrumentation Engineering, Faculty of Engineering & Technology Annamalai

More information

Attitude Control Strategy for HAUSAT-2 with Pitch Bias Momentum System

Attitude Control Strategy for HAUSAT-2 with Pitch Bias Momentum System SSC06-VII-5 Attitude Control Strategy for HAUSAT-2 with Pitch Bias Momentum System Young-Keun Chang, Seok-Jin Kang, Byung-Hoon Lee, Jung-on Choi, Mi-Yeon Yun and Byoung-Young Moon School of Aerospace and

More information

Mathematical Models for the Triaxial Attitude Control Testbed

Mathematical Models for the Triaxial Attitude Control Testbed Draft Article (For Engineering Journals) Mathematical Models for the Triaxial Attitude Control Testbed Sangbum Cho, Jinglai Shen, N. Harris McClamroch Department of Aerospace Engineering University of

More information

FIBER OPTIC GYRO-BASED ATTITUDE DETERMINATION FOR HIGH- PERFORMANCE TARGET TRACKING

FIBER OPTIC GYRO-BASED ATTITUDE DETERMINATION FOR HIGH- PERFORMANCE TARGET TRACKING FIBER OPTIC GYRO-BASED ATTITUDE DETERMINATION FOR HIGH- PERFORMANCE TARGET TRACKING Elias F. Solorzano University of Toronto (Space Flight Laboratory) Toronto, ON (Canada) August 10 th, 2016 30 th AIAA/USU

More information

7. The gyroscope. 7.1 Introduction. 7.2 Theory. a) The gyroscope

7. The gyroscope. 7.1 Introduction. 7.2 Theory. a) The gyroscope K 7. The gyroscope 7.1 Introduction This experiment concerns a special type of motion of a gyroscope, called precession. From the angular frequency of the precession, the moment of inertia of the spinning

More information

A FORCE BALANCE TECHNIQUE FOR MEASUREMENT OF YOUNG'S MODULUS. 1 Introduction

A FORCE BALANCE TECHNIQUE FOR MEASUREMENT OF YOUNG'S MODULUS. 1 Introduction A FORCE BALANCE TECHNIQUE FOR MEASUREMENT OF YOUNG'S MODULUS Abhinav A. Kalamdani Dept. of Instrumentation Engineering, R. V. College of Engineering, Bangalore, India. kalamdani@ieee.org Abstract: A new

More information

Internal Torques and Forces in Gyrostats with Magnetically Suspended Rotors

Internal Torques and Forces in Gyrostats with Magnetically Suspended Rotors Internal Torques and Forces in Gyrostats with Magnetically Suspended Rotors by Marcus Carl Pressl Thesis submitted to the Faculty of the Virginia Polytechnic Institute and State University in partial fulfillment

More information

Estimation of Tire-Road Friction by Tire Rotational Vibration Model

Estimation of Tire-Road Friction by Tire Rotational Vibration Model 53 Research Report Estimation of Tire-Road Friction by Tire Rotational Vibration Model Takaji Umeno Abstract Tire-road friction is the most important piece of information used by active safety systems.

More information

is acting on a body of mass m = 3.0 kg and changes its velocity from an initial

is acting on a body of mass m = 3.0 kg and changes its velocity from an initial PHYS 101 second major Exam Term 102 (Zero Version) Q1. A 15.0-kg block is pulled over a rough, horizontal surface by a constant force of 70.0 N acting at an angle of 20.0 above the horizontal. The block

More information

Laws of gyroscopes / cardanic gyroscope

Laws of gyroscopes / cardanic gyroscope Principle If the axis of rotation of the force-free gyroscope is displaced slightly, a nutation is produced. The relationship between precession frequency or nutation frequency and gyrofrequency is examined

More information

CEE 271: Applied Mechanics II, Dynamics Lecture 25: Ch.17, Sec.4-5

CEE 271: Applied Mechanics II, Dynamics Lecture 25: Ch.17, Sec.4-5 1 / 36 CEE 271: Applied Mechanics II, Dynamics Lecture 25: Ch.17, Sec.4-5 Prof. Albert S. Kim Civil and Environmental Engineering, University of Hawaii at Manoa Date: 2 / 36 EQUATIONS OF MOTION: ROTATION

More information

Adaptive Backstepping Control for Optimal Descent with Embedded Autonomy

Adaptive Backstepping Control for Optimal Descent with Embedded Autonomy Adaptive Backstepping Control for Optimal Descent with Embedded Autonomy Maodeng Li, Wuxing Jing Department of Aerospace Engineering, Harbin Institute of Technology, Harbin, Heilongjiang, 150001, China

More information

c 2009 John Gregory Warner

c 2009 John Gregory Warner c 2009 John Gregory Warner ATTITUDE DETERMINATION AND CONTROL OF NANO-SATELLITES BY JOHN GREGORY WARNER THESIS Submitted in partial fulfillment of the requirements for the degree of Master of Science in

More information

Recap: Solid Rotational Motion (Chapter 8) displacement velocity acceleration Newton s 2nd law τ = I.α N.s τ = F. l moment of inertia mass size

Recap: Solid Rotational Motion (Chapter 8) displacement velocity acceleration Newton s 2nd law τ = I.α N.s τ = F. l moment of inertia mass size Recap: Solid Rotational Motion (Chapter 8) We have developed equations to describe rotational displacement θ, rotational velocity ω and rotational acceleration α. We have used these new terms to modify

More information

Lecture AC-1. Aircraft Dynamics. Copy right 2003 by Jon at h an H ow

Lecture AC-1. Aircraft Dynamics. Copy right 2003 by Jon at h an H ow Lecture AC-1 Aircraft Dynamics Copy right 23 by Jon at h an H ow 1 Spring 23 16.61 AC 1 2 Aircraft Dynamics First note that it is possible to develop a very good approximation of a key motion of an aircraft

More information

AA 528 Spacecraft Dynamics and Control. Mehran Mesbahi Aeronautics & Astronautics Winter 2017 University of Washington

AA 528 Spacecraft Dynamics and Control. Mehran Mesbahi Aeronautics & Astronautics Winter 2017 University of Washington AA 528 Spacecraft Dynamics and Control Mehran Mesbahi Aeronautics & Astronautics Winter 2017 University of Washington Spacecraft dynamics and control What is this class all about? what is in the name?

More information

Optimal Fault-Tolerant Configurations of Thrusters

Optimal Fault-Tolerant Configurations of Thrusters Optimal Fault-Tolerant Configurations of Thrusters By Yasuhiro YOSHIMURA ) and Hirohisa KOJIMA, ) ) Aerospace Engineering, Tokyo Metropolitan University, Hino, Japan (Received June st, 7) Fault tolerance

More information

Lecture 9 - Rotational Dynamics

Lecture 9 - Rotational Dynamics Lecture 9 - Rotational Dynamics A Puzzle... Angular momentum is a 3D vector, and changing its direction produces a torque τ = dl. An important application in our daily lives is that bicycles don t fall

More information

Analytical Mechanics. of Space Systems. tfa AA. Hanspeter Schaub. College Station, Texas. University of Colorado Boulder, Colorado.

Analytical Mechanics. of Space Systems. tfa AA. Hanspeter Schaub. College Station, Texas. University of Colorado Boulder, Colorado. Analytical Mechanics of Space Systems Third Edition Hanspeter Schaub University of Colorado Boulder, Colorado John L. Junkins Texas A&M University College Station, Texas AIM EDUCATION SERIES Joseph A.

More information

Chapter 8 Rotational Motion and Equilibrium. 1. Give explanation of torque in own words after doing balance-the-torques lab as an inquiry introduction

Chapter 8 Rotational Motion and Equilibrium. 1. Give explanation of torque in own words after doing balance-the-torques lab as an inquiry introduction Chapter 8 Rotational Motion and Equilibrium Name 1. Give explanation of torque in own words after doing balance-the-torques lab as an inquiry introduction 1. The distance between a turning axis and the

More information

Hysteresis Nutation Damper for Spin Satellite

Hysteresis Nutation Damper for Spin Satellite Hysteresis Nutation Damper for Spin Satellite Hamed Shahmohamadi Ousaloo * Send Orders for Reprints to reprints@benthamscience.net The Open Aerospace Engineering Journal, 2013, 6, 1-5 1 Open Access Space

More information

Exercise Torque Magnitude Ranking Task. Part A

Exercise Torque Magnitude Ranking Task. Part A Exercise 10.2 Calculate the net torque about point O for the two forces applied as in the figure. The rod and both forces are in the plane of the page. Take positive torques to be counterclockwise. τ 28.0

More information

Phys101 Lectures 19, 20 Rotational Motion

Phys101 Lectures 19, 20 Rotational Motion Phys101 Lectures 19, 20 Rotational Motion Key points: Angular and Linear Quantities Rotational Dynamics; Torque and Moment of Inertia Rotational Kinetic Energy Ref: 10-1,2,3,4,5,6,8,9. Page 1 Angular Quantities

More information

A Miniaturized Satellite Attitude Determination and Control System with Autonomous Calibration Capabilities

A Miniaturized Satellite Attitude Determination and Control System with Autonomous Calibration Capabilities A Miniaturized Satellite Attitude Determination and Control System with Autonomous Calibration Capabilities Sanny Omar Dr. David Beale Dr. JM Wersinger Introduction ADACS designed for CubeSats CubeSats

More information

PLANAR KINETIC EQUATIONS OF MOTION (Section 17.2)

PLANAR KINETIC EQUATIONS OF MOTION (Section 17.2) PLANAR KINETIC EQUATIONS OF MOTION (Section 17.2) We will limit our study of planar kinetics to rigid bodies that are symmetric with respect to a fixed reference plane. As discussed in Chapter 16, when

More information

MECH 3140 Final Project

MECH 3140 Final Project MECH 3140 Final Project Final presentation will be held December 7-8. The presentation will be the only deliverable for the final project and should be approximately 20-25 minutes with an additional 10

More information

Lab 11: Rotational Dynamics

Lab 11: Rotational Dynamics Lab 11: Rotational Dynamics Objectives: To understand the relationship between net torque and angular acceleration. To understand the concept of the moment of inertia. To understand the concept of angular

More information

LAWS OF GYROSCOPES / CARDANIC GYROSCOPE

LAWS OF GYROSCOPES / CARDANIC GYROSCOPE LAWS OF GYROSCOPES / CARDANC GYROSCOPE PRNCPLE f the axis of rotation of the force-free gyroscope is displaced slightly, a nutation is produced. The relationship between precession frequency or nutation

More information

Lezione 9 30 March. Scribes: Arianna Marangon, Matteo Vitturi, Riccardo Prota

Lezione 9 30 March. Scribes: Arianna Marangon, Matteo Vitturi, Riccardo Prota Control Laboratory: a.a. 2015/2016 Lezione 9 30 March Instructor: Luca Schenato Scribes: Arianna Marangon, Matteo Vitturi, Riccardo Prota What is left to do is how to design the low pass pole τ L for the

More information