Attitude Control Subsystem Design of the Stable and Highly Accurate Pointing Earth-Imager

Total Page:16

File Type:pdf, Size:1020Kb

Attitude Control Subsystem Design of the Stable and Highly Accurate Pointing Earth-Imager Attitude Control Subsystem Design of the Stable and Highly Accurate Pointing Earth-imager A MSc Thesis By David Ju in partial fulfillment of the requirements for the degree of Master of Science in Aerospace Engineering at the Delft University of Technology Department of Space Engineering 5th October 2017 Supervisor Dr.ir. J.M. Kuiper Committee Members Dr. A. Cervone ir. B.C. Root Abbreviations ACS Attitude Control Subsystem ADCS Attitude Determination and Control Subsystem ARE Algebraic Ricatti Equation ATS Attitude Thruster Subsystem CMG Control Moment Gyro ConOps Concept of Operations COTS Commercial off the shelf EO Earth Observation FMS1 Full Major Spinup FMS2 Full Minor Spinup FOV Field of View IAGA International Association of Geomagnetism and Aeronomy IFOV Instantaneous Field of View IGRF12 International Geomagnetic Reference Field 12th generation LEO Low Earth Orbit LQR Linear Quadratic Regulator MEMS microelectromechanical system MSAFE Marshall Solar Activity Future Estimates (Model) MSFC Marshall Space Flight Center MT Magnetorquer MTF Modulation Transfer Function MW Momentum Wheel MWTS Momentum Wheel Torquing Subsystem NASA National Aeronautics and Space Administration NRLMSISE00 Naval Research Laboratory Mass Spectrometer and Incoherent Scatter radar Exosphere (2001 Model) PPL Precession Phase Lock PS Partial Spinup RW Reaction Wheel SHAPE Stable and Highly Accurate Pointing Earth-imager SMC Sliding Mode Control SMCS Sliding Mode Control Spinup SSO Sun Synchronous Orbit 2 TBD To Be Determined UTC Coordinated Universal Time VLEO Very Low Earth Orbit Nomenclature η Nutation Angle [deg] λ Longitude [deg] µ Pointing Error [rad] −7 -1 µ0 Vacuum Magnetic Permeability [4 π · 10 T m A ] 3 -2 µE Gravitational Parameter of Earth [398 600 km s ] ! Angular Body Rate Column Vector [rad s-1] Ωp Precession Frequency [rad/s] -1 !s Relative Rotor Angular Velocity Around the Spin Axis [rad s ] φ Latitude [deg] ρ Total Air Mass Density [kg m-3] -3 ρm Material Density [kg m ] τ External Torque [Nm] ξ Damper Displacement [m] A Wetted Surface Area [m2] a Semi-major Axis [km] B Magnetic Flux Density [T] b Initial Damper Mass Location to Center of Mass Column Vector [m] -1 cd Damping Coefficient [kg s m ] CD Drag Coefficient [-] FT Thrust [N] ga Spinup Torque [Nm] h Altitude [km] H Angular Momentum Column Vector [N m s] Hs Rotor Angular Momentum [N m s] I Mass Moment of Inertia Matrix [kg m2] 2 Is Rotor Moment of Inertia Around the Spin Axis [kg m ] -1 kd Spring Stiffness [kg m ] 3 m Mass [kg] 2 MA Dipole Moment Vector of the Magnetorquers [A m ] 22 2 ME Earth’s Magnetic Moment Vector [8 · 10 A m ] 2 MM Spacecraft Magnetic Moment Vector [A m ] md Damper Mass [kg] n Mean Motion [rad s-1] n Spin Axis Column Vector [-] p Linear Momentum Vector [kg m s-1] -1 pn Linear Momentum of Damper Mass [kg m s ] T Rotational Kinetic Energy [J] tm Maintenance Operation Time [s] tn Nominal Operation Time [s] 4 Abstract As technology improves, increasingly higher resolution payload can be achieved using Cubesats for Earth observation. The diffraction limit prevents the resolution to up to a few meters for these missions and are confined to Very Low Earth Orbits (VLEO). At these altitudes, strong disturbances act on the system, limiting its lifetime and the pointing capabilities of CubeSats. As a solution, the Department of Space Engineering at the Delft University of Technology has proposed a 6 unit CubeSat named the Stable and Highly Accurate Pointing Earth-imager (SHAPE) orbiting at a Sun synchronous VLEO which uses a momentum wheel to passively stabilize the system against the external environment within a competitive cost of less than 500 000 e. By utilizing the dual-spin stabilization concept, composed of a stable platform and a spinning rotor, it is expected to perform pointing missions of less than 1 degree. In this thesis, the SHAPE concept has been revisited and further developed based on the work of Kuiper and Dolkens to conduct whether these types of missions are feasible within the aspect of the Attitude Determination and Control Subsystem (ADCS). This thesis covers the base of this subsystem approached from a top-down methodology; designed from the final nominal mission mode to the detumbling mode on a system level. The ADCS design will consist of a momentum wheel which has been determined to have an angular momentum of 1 Nms. This value is based on a prediction of the worst-case atmospheric density of the next solar cycle. The design point, at which the momentum wheel has been sized, has been taken at 90% of SHAPE’s lifetime after several design iterations. Hereby, the last 10% of the mission has been partially forfeited with degraded performances due to the exponential increase in disturbances acting on the spacecraft at lower altitudes. As therefore, the mass and size of the momentum wheel has been reduced with 41% and 20%, respectively. To re-align the angular momentum vector within the 1 degree pointing requirement, a set of magnetorquers with a dipole moment of 0.5 Am2 has been chosen due to their low power consumption, mass, cost, and high reliability while capable of producing sufficient torque. Also, a damper is to be integrated as it provides the system asymptotic reduction of the transverse momenta, thus increasing the image quality without expenditure of additional power. To reach the nominal mission observation state, several momentum wheel spinup strategies have been investigated. Based on a trade-off between three spinup concepts, it was concluded that the major axis spinup is most suited. This type is initiated after the spacecraft as a whole has attained an angular momentum equivalent to that of the desired end value of the momentum wheel. Then, a constant rotor torque is applied, providing a momentum transfer from the platform to the rotor. The disadvantage of this spinup procedure is that the system’s solar panels are aligned parallel to the orbital plane, meaning that power cannot be generated and batteries are required during the spinup. Despite this, it was found that after completing the spinup, the transverse angular momenta was minimized to marginal values in contrast to the other spins. The inclusion of the passive damper during the major axis spin further improves the ability of reducing the transverse momentum as the damper’s dissipative energy property adds an asymptotic attraction at the point of lowest energy, located at the spin axis near the end of the spinup. The all-spun state is achieved using a set of thrusters. This choice was taken as the magnetorquers was found not to deliver sufficient torque. From the detumbling analysis, it was concluded that the magnetorquers are able to reduce the tumbling rates with magnitudes of up to 35 deg/s to mean motion values in less than an orbit using a static gain B-dot controller. Imperfections in the momentum wheel can cause static and dynamic imbalance, imparting internal disturbances to the system which affects the image quality detrimentally. Therefore, isolators are to be integrated within the momentum wheel suspension subsystem. If these disturbances can be negated using isolators, it can be expected that the pointing error will stay within one degree and attitude stability can be achieved at least until the design altitude of 280 km. However, the analysis and design of the isolators have yet to be done and thus the attainability of the pointing and image quality requirements are still inconclusive. 5 6 "Life is the sum of all your choices." - Albert Camus 7 8 Preface From my youth, I was always fascinated in rockets, planets and the universe (and also insects for which my curiosity to it has vanished). Pursuing science was very obvious. The interest of space and pursue to it were not during my lifetime. At my final years of high school, my carrier decision had to be made and was divided into either medicine or aerospace engineering; to help people or go into the direction of my own interest. This decision was tough, but I decided to pursue in aerospace engineering at Delft University of Technology mainly as a challenge. Halfway though my bachelor studies, aerospace engineering had not been motivating for me and pursuing this seemed to have been disappointing. Doubt was in my mind. This changed at the design synthesis exercise. Focusing more on the space and especially on the attitude control system of the spacecraft has awoken my fascination in space and has enlightened me to further pursue to do my master’s degree in space engineering. To keep thinking about what to do and what would have been if I have chosen a different path is a thought of futility as life is continuous and flowing in a single direction. Or as Albert Camus, a philosopher of the Absurd, has said; "You will never be happy if you continue to search for what happiness consists of. You will never live if you are looking for the meaning of life." I would like to thank my supervisor Hans Kuiper for the subject of SHAPE and his pragmatic approach towards engineering. This subject has greatly introduced me to spinning spacecraft (which I thought to be obsolete for satellites) and its intriguing complex rotational motions. Furthermore, I am especially grateful for my parents and brother for supporting me throughout my academic life with their love for which I dedicate this thesis to. 9 Contents 1 Introduction 17 2 System Objective 19 2.1 Case Study . 19 2.2 System Requirements . 20 2.3 Control Modes . 21 2.3.1 Control Mode Requirements . 22 2.3.2 Modulation Transfer Function Requirement . 24 2.4 Design Methodology .
Recommended publications
  • Longitudinal & Lateral Directional Short Course
    1 Longitudinal & Lateral Directional Short Course Flight One – Effects of longitudinal stability and control characteristics on handling qualities Background: In this flight training exercise we will examine how longitudinal handling qualities are affected by three important variables that are inherent in a given aircraft design. They are: Static longitudinal stability Dynamic longitudinal stability Elevator control effectiveness As you will recall from your classroom briefings, longitudinal stability is responsible for the frequency response to a disturbance, which can be caused by the atmosphere or an elevator control input. It may be described by two longitudinal oscillatory modes of motion: A Long term response (Phugoid), which is a slow or low frequency oscillation, occurring at a relatively constant angle of attack with altitude and speed variations. This response largely affects the ability to trim for a steady state flight condition. A short term response where a higher frequency oscillation occurs at a relatively constant speed and altitude, but with a change in angle of attack. This response is associated with maneuvering the aircraft to accomplish a closed loop task, such as an instrument approach procedure. If static stability is positive; The long and short period responses will either be convergent or neutral (oscillations) depending on dynamic stability If neutral; The long period will no longer be oscillatory and short period pitch responses will decay to a pitch rate response proportional to the amount of elevator input; If slightly negative (Equivalent of moving CG behind the stick fixed neutral point); In the long period, elevator stick position will reverse, i.e., as speed increases a pull will be required on the elevator followed by a push, and as speed decreases, a push will be required followed by a pull The short period responses will result in a continuous divergence from the trim state.
    [Show full text]
  • Introduction to Aircraft Stability and Control Course Notes for M&AE 5070
    Introduction to Aircraft Stability and Control Course Notes for M&AE 5070 David A. Caughey Sibley School of Mechanical & Aerospace Engineering Cornell University Ithaca, New York 14853-7501 2011 2 Contents 1 Introduction to Flight Dynamics 1 1.1 Introduction....................................... 1 1.2 Nomenclature........................................ 3 1.2.1 Implications of Vehicle Symmetry . 4 1.2.2 AerodynamicControls .............................. 5 1.2.3 Force and Moment Coefficients . 5 1.2.4 Atmospheric Properties . 6 2 Aerodynamic Background 11 2.1 Introduction....................................... 11 2.2 Lifting surface geometry and nomenclature . 12 2.2.1 Geometric properties of trapezoidal wings . 13 2.3 Aerodynamic properties of airfoils . ..... 14 2.4 Aerodynamic properties of finite wings . 17 2.5 Fuselage contribution to pitch stiffness . 19 2.6 Wing-tail interference . 20 2.7 ControlSurfaces ..................................... 20 3 Static Longitudinal Stability and Control 25 3.1 ControlFixedStability.............................. ..... 25 v vi CONTENTS 3.2 Static Longitudinal Control . 28 3.2.1 Longitudinal Maneuvers – the Pull-up . 29 3.3 Control Surface Hinge Moments . 33 3.3.1 Control Surface Hinge Moments . 33 3.3.2 Control free Neutral Point . 35 3.3.3 TrimTabs...................................... 36 3.3.4 ControlForceforTrim. 37 3.3.5 Control-force for Maneuver . 39 3.4 Forward and Aft Limits of C.G. Position . ......... 41 4 Dynamical Equations for Flight Vehicles 45 4.1 BasicEquationsofMotion. ..... 45 4.1.1 ForceEquations .................................. 46 4.1.2 MomentEquations................................. 49 4.2 Linearized Equations of Motion . 50 4.3 Representation of Aerodynamic Forces and Moments . 52 4.3.1 Longitudinal Stability Derivatives . 54 4.3.2 Lateral/Directional Stability Derivatives .
    [Show full text]
  • Static Stability and Control
    CHAPTER 2 Static Stability and Control "lsn't it astonishing that all these secrets have been preserved for so many years just so that we could discover them!" Orville Wright, June 7, 1903 2.1 HISTORICAL PERSPECTIVE By the start of the 20th century, the aeronautical community had solved many of the technical problems necessary for achieving powered flight of a heavier-than-air aircraft. One problem still beyond the grasp of these early investigators was a lack of understanding of the relationship between stability and control as well as the influence of the pilot on the pilot-machine system. Most of the ideas regarding stability and control came from experiments with uncontrolled hand-launched gliders. Through such experiments, it was quickly discovered that for a successful flight the glider had to be inherently stable. Earlier aviation pioneers such as Albert Zahm in the United States, Alphonse Penaud in France, and Frederick Lanchester in England contributed to the notion of stability. Zahm, however, was the first to correctly outline the requirements for static stability in a paper he presented in 1893. In his paper, he analyzed the conditions necessary for obtaining a stable equilibrium for an airplane descending at a constant speed. Figure 2.1 shows a sketch of a glider from Zahm's paper. Zahm concluded that the center of gravity had to be in front of the aerodynamic force and the vehicle would require what he referred to as "longitudinal dihedral" to have a stable equilibrium point. In the terminology of today, he showed that, if the center of gravity was ahead of the wing aerodynamic center, then one would need a reflexed airfoil to be stable at a positive angle of attack.
    [Show full text]
  • Concept of Moving Centre of Gravity for Improved Directional Stability for Automobiles
    IJIRST –International Journal for Innovative Research in Science & Technology| Volume 2 | Issue 11 | April 2016 ISSN (online): 2349-6010 Concept Of Moving Centre of Gravity for Improved Directional Stability for Automobiles - Simulation Joseph Sebastian Siyad S UG Student UG Student Department of Mechanical Engineering Department of Mechanical Engineering Saintgits College of Engineering Saintgits College of Engineering Subin Antony Jose Ton Devasia UG Student UG Student Department of Mechanical Engineering Department of Mechanical Engineering Saintgits College of Engineering Saintgits College of Engineering Prof. Sajan Thomas Professor Department of Mechanical Engineering Saintgits College of Engineering Abstract This paper is a study based on the implementation of a new concept in AUTOMOBILE which will help in improving the directional stability and handling characteristics of vehicle. The purpose of this study is to analyze the influence of position of CENTRE OF GRAVITY of a vehicle in its stability in accordance with YAW MOTION, ROLL MOTION, UNDER STEER and OVER STEER. The concept is to implement a mechanism which can bring SHIFTING OF C.G in automobile, as per the conditions. The influence of position of C.G is much bigger for the balancing of forces in dynamic stability of the vehicle. The concept of moving C.G will help to acquire this added stability to the vehicle even in the worst conditions.The directional stability of a vehicle is influenced by the steering angle and slip angle of the tire to an extent. It is possible to have a variation in these values by the shifting of CG. The designing of a convenient mechanism which helps in achieving the movement of the mass (either by pumping a high density fluid or my movement of a solid block by mechanical linkage) is to be done and have to be tested in a real time vehicle.
    [Show full text]
  • Stability and Control
    Stability and Control AE460 Aircraft Design Greg Marien Lecturer Introduction Complete Aircraft wing, tail and propulsion configuration, Mass Properties, including MOIs Non-Dimensional Derivatives (Roskam) Dimensional Derivatives (Etkin) Calculate System Matrix [A] and eigenvalues and eigenvectors Use results to determine stability (Etkin) Reading: Nicolai - CH 21, 22 & 23 Roskam – VI, CH 8 & 10 Other references: MIL-STD-1797/MIL-F-8785 Flying Qualities of Piloted Aircraft Airplane Flight Dynamics Part I (Roskam) 2 What are the requirements? Evaluate your aircraft for meeting the stability requirements See SRD (Problem Statement) for values • Flight Condition given: – Airspeed: M = ? – Altitude: ? ft. – Standard atmosphere – Configuration: ? – Fuel: ?% • Longitudinal Stability: – CmCGα < 0 at trim condition – Short period damping ratio: ? – Phugoid damping ratio: ? • Directional Stability: – Dutch roll damping ratio: ? – Dutch roll undamped natural frequency: ? – Roll-mode time constant: ? – Spiral time to double amplitude: ? 3 Derivatives • For General Equations of Unsteady Motions, reference Etkin, Chapter 4 • Assumptions – Aircraft configuration finalized – All mass properties are known, including MOI – Non-Dimensional Derivatives completed for flight condition analyzed – Aircraft is a rigid body – Symmetric aircraft across BL0, therefore Ixy=Iyz = 0 – Axis of spinning rotors are fixed in the direction of the body axis and have constant angular speed – Assume a small disturbance • Results in the simplified Linear Equations of Motion…
    [Show full text]
  • Assessment of Tire Features for Modeling Vehicle Stability in Case of Vertical Road Excitation
    applied sciences Article Assessment of Tire Features for Modeling Vehicle Stability in Case of Vertical Road Excitation Vaidas Lukoševiˇcius*, Rolandas Makaras and Andrius Dargužis Faculty of Mechanical Engineering and Design, Kaunas University of Technology, Studentu˛Str. 56, 44249 Kaunas, Lithuania; [email protected] (R.M.); [email protected] (A.D.) * Correspondence: [email protected] Abstract: Two trends could be observed in the evolution of road transport. First, with the traffic becoming increasingly intensive, the motor road infrastructure is developed; more advanced, greater quality, and more durable materials are used; and pavement laying and repair techniques are im- proved continuously. The continued growth in the number of vehicles on the road is accompanied by the ongoing improvement of the vehicle design with the view towards greater vehicle controllability as the key traffic safety factor. The change has covered a series of vehicle systems. The tire structure and materials used are subject to continuous improvements in order to provide the maximum possi- ble grip with the road pavement. New solutions in the improvement of the suspension and driving systems are explored. Nonetheless, inevitable controversies have been encountered, primarily, in the efforts to combine riding comfort and vehicle controllability. Practice shows that these systems perform to a satisfactory degree only on good quality roads, as they have been designed specifically for the latter. This could be the cause of the more complicated car control and accidents on the lower-quality roads. Road ruts and local unevenness that impair car stability and traffic safety are not Citation: Lukoševiˇcius,V.; Makaras, avoided even on the trunk roads.
    [Show full text]
  • Advanced Problems of Lateral-Directional Dynamics
    12/4/18 Advanced Problems of Lateral- Directional Dynamics Robert Stengel, Aircraft Flight Dynamics MAE 331, 2018 Learning Objectives • 4th-order dynamics – Steady-state response to control – Transfer functions – Frequency response – Root locus analysis of parameter variations • Residualization Flight Dynamics 595-627 Copyright 2018 by Robert Stengel. All rights reserved. For educational use only. http://www.princeton.edu/~stengel/MAE331.html 1 http://www.princeton.edu/~stengel/FlightDynamics.html Stability-Axis Lateral-Directional Equations With idealized aileron and rudder effects (i.e., NδA = LδR = 0) ⎡ ⎤ Nr Nβ N p 0 ⎡ Δr!(t) ⎤ ⎢ ⎥⎡ Δr(t) ⎤ ⎡ ~ 0 N ⎤ ⎢ ⎥ Y ⎢ ⎥ δ R ! ⎢ β g ⎥ ⎢ ⎥ ⎢ Δβ(t) ⎥ −1 0 ⎢ Δβ(t) ⎥ 0 0 ⎡ Δδ A ⎤ = ⎢ V V ⎥ + ⎢ ⎥ ⎢ ⎥ ⎢ N N ⎥⎢ ⎥ ⎢ ⎥⎢ ⎥ Δp!(t) Δp(t) Lδ A ~ 0 ⎣ Δδ R ⎦ ⎢ ⎥ ⎢ L L L 0 ⎥⎢ ⎥ ⎢ ⎥ ⎢ Δφ!(t) ⎥ r β p Δφ(t) 0 0 ⎣ ⎦ ⎢ ⎥⎣⎢ ⎦⎥ ⎣⎢ ⎦⎥ ⎢ 0 0 1 0 ⎥ ⎣ ⎦ " % " % Δx1 " Δr % Yaw Rate Perturbation $ ' $ ' $ ' " % " % $ Δx2 ' Δβ $ Sideslip Angle Perturbation ' Δu1 " Δδ A % Aileron Perturbation = $ ' = $ ' = = $ ' $ ' $ p ' $ ' $ ' Δx3 Δ Roll Rate Perturbation Δu Δδ R Rudder Perturbation $ ' $ ' $ ' #$ 2 &' # & #$ &' $ Δx ' Δφ $ Roll Angle Perturbation ' # 4 & #$ &' # & 2 1 12/4/18 Lateral-Directional Characteristic Equation 4 ⎛ Yβ ⎞ 3 Δ LD (s) = s + ⎜ Lp + Nr + ⎟ s ⎝ VN ⎠ ⎡ Y Y ⎤ N L N L β N ⎛ β L ⎞ s2 + ⎢ β − r p + p V + r ⎜ V + p ⎟ ⎥ ⎣ N ⎝ N ⎠ ⎦ ⎡Yβ g ⎤ + (Lr N p − Lp Nr ) + Lβ N p − s ⎣⎢ VN ( VN )⎦⎥ g + Lβ Nr − Lr Nβ VN ( ) 4 3 2 = s + a3s + a2s + a1s + a0 = 0 Typically factors into real spiral and roll roots and an oscillatory
    [Show full text]
  • X-29A Lateral–Directional Stability and Control Derivatives Extracted from High-Angle-Of- Attack Flight Data
    NASA Technical Paper 3664 December 1996 X-29A Lateral–Directional Stability and Control Derivatives Extracted From High-Angle-of- Attack Flight Data Kenneth W. Iliff Kon-Sheng Charles Wang NASA Technical Paper 3664 1996 X-29A Lateral–Directional Stability and Control Derivatives Extracted From High-Angle-of- Attack Flight Data Kenneth W. Iliff Dryden Flight Research Center Edwards, California Kon-Sheng Charles Wang SPARTA, Inc. Lancaster, California National Aeronautics and Space Administration Office of Management Scientific and Technical Information Program CONTENTS Page ABSTRACT . 1 NOMENCLATURE . 1 Acronyms . 1 Symbols . 1 INTRODUCTION . 3 FLIGHT PROGRAM OVERVIEW . 4 VEHICLE DESCRIPTION . 5 INSTRUMENTATION AND DATA ACQUISITION . 7 PREDICTIONS AND ENVELOPE EXPANSION METHODS . 8 PARAMETER IDENTIFICATION METHODOLOGY . 9 RESULTS AND DISCUSSION. 13 Sideslip Derivatives . 14 Aileron Derivatives. 15 Rudder Derivatives . 16 Rotary Derivatives . 16 Aerodynamic and Instrumentation Biases . 17 CONCLUDING REMARKS . 18 REFERENCES . 19 FIGURES 1. X-29A aircraft, number 2 . 22 2. Three-view drawing of the X-29A showing major dimensions . 23 3. The maximum likelihood estimation concept with state and measurement noise . 24 4. Time-history data for a typical high-AOA, lateral–directional, PID maneuver . 25 5. Sideslip derivatives as functions of AOA . 28 6. Aileron derivatives as functions of AOA . 29 7. Rudder derivatives as functions of AOA . 31 8. Rotary derivatives as functions of AOA . 32 9. Aerodynamic and instrumentation biases as functions of AOA . 34 iii ABSTRACT The lateral–directional stability and control derivatives of the X-29A number 2 are extracted from flight data over an angle-of-attack range of 4° to 53° using a parameter identification algorithm.
    [Show full text]
  • Stability and Control Flight Testing of the Dassault Falcon 10/100 By
    Stability and Control Flight Testing of the Dassault Falcon 10/100 by Andres Mauricio Alarcon Vega A thesis submitted to the College of Engineering and Science of Florida Institute of Technology in partial fulfillment of the requirements for the degree of Master of Science in Flight Test Engineering Melbourne, Florida May 2021 We the undersigned committee hereby approve the attached thesis, “Stability and Control Flight Testing of the Dassault Falcon 10/100” by Andres Mauricio Alarcon Vega _________________________________________________ Brian A. Kish, Ph.D. Associate Professor Aerospace, Physics and Space Sciences Major Advisor _________________________________________________ Markus Wilde, Dr.-Ing. Associate Professor Aerospace, Physics and Space Sciences Committee Member _________________________________________________ Isaac Silver, Ph.D. Test Pilot Energy Management Aerospace LLC Committee Member _________________________________________________ David Fleming, Ph.D. Associate Professor and Department Head Aerospace, Physics and Space Sciences Abstract Title: Stability and Control Flight Testing of the Dassault Falcon 10/100 Author: Andres Mauricio Alarcon Vega Advisor: Brian A. Kish, Ph.D. The Falcon 10/100 is a transport category aircraft developed by Dassault Aviation in 1971. Production of the aircraft ceased in 1989, but it remains available on the secondhand market. Certification for these types of aircraft follow FAR Part 25 of the code of federal regulations. Aircraft stability and control flying qualities are dependent on the mission profile and intended use case of the aircraft. External factors, such as turbulence, are relevant for transport category aircraft because poor stability could affect the flying characteristics and result in an unpleasant ride. On the other hand, in a trimmed condition, an aircraft with strong positive stability has a greater resistance to disturbances.
    [Show full text]
  • Electronic Stability Control Systems
    Transport Canada Transports Canada Safety and Security Sécurité et sûreté Road Safety Sécurité routière Standards and Regulations Division TECHNICAL STANDARDS DOCUMENT No. 126, Revision 0 Electronic Stability Control Systems The text of this document is based on Federal Motor Vehicle Safety Standard No. 126, Electronic Stability Control Systems, as published in the U.S. Code of Federal Regulations, Title 49, Part 571, revised as of October 1, 2007, as well as the Final Rule published in the Federal Register on September 22, 2008 (Vol. 73, No. 184, p. 54526). Effective Date: Month ##, 200# Mandatory Compliance Date: September 1, 2011 Standards Research and Development Branch Road Safety and Motor Vehicle Regulation Directorate TRANSPORT CANADA Ottawa, Ontario K1A 0N5 Technical Standards Document Number 126, Revision 0 Electronic Stability Control Systems (Ce document est aussi disponible en français.) Introduction As defined by section 12 of the Motor Vehicle Safety Act, a Technical Standards Document (TSD) is a document that reproduces an enactment of a foreign government (e.g. a Federal Motor Vehicle Safety Standard issued by the U.S. National Highway Traffic Safety Administration). According to the Act, the Motor Vehicle Safety Regulations may alter or override some provisions contained in a TSD or specify additional requirements; consequently, it is advisable to read a TSD in conjunction with the Act and its counterpart Regulation. As a guide, where the corresponding Regulation contains additional requirements, footnotes indicate the amending subsection number. TSDs are revised from time to time in order to incorporate amendments made to the reference document, at which time a Notice of Revision is published in the Canada Gazette, Part I.
    [Show full text]
  • Research Requirements for Determining Car Handling Characteristics
    Research Requirements for Determining Car Handling Characteristics JOHN VERSACE and LYMAN M. FORBES, Ford Motor Company Distinction is made between handling, which is the behavior of a car-man combination in actual driving, and other variables, such as vehicle directional response properties and vehicle component designs. The relation between car-man handling be­ havior and safety (as indicated by the frequency and extent of accident injuries and fatalities) is discernible in accident sta­ tistics. But the relation of the car-only portion (its directional response properties) to the frequency of accidents and conse­ quently to the extent of injuries and fatalities is largely unknown. Furthermore, the relation of the vehicle response properties to actual handling in the driving population is poorly known, partly because of difficulties in defining handling with sufficient objectivity to allow for its measurement. The paper briefly summarizes present practice in the development of car design to a handling criterion, and presents some basic considerations for research studies that will relate handling behavior to vehicle properties. A history of the recent interest in relating handling to vehicle properties is also included. •IF one reads the sports car magazines it may seem that a lot is known about car han­ dling and that performance requirements for handling could be set up easily. In a sense this is true because vehicle planners do indeed specify handling requirements and vehi­ cles are designed and developed to meet them. However, two aspects of the matter cause difficulty. First, there is no sure trans­ formation of what is now mainly subjective knowledge obtained through long and intimate experience into quantitative, objective, instrumental procedures for unambiguous mea­ surement and assessment of handling quality.
    [Show full text]
  • Axes and Derivatives
    Flightlab Ground School 1. Axes and Derivatives Copyright Flight Emergency & Advanced Maneuvers Training, Inc. dba Flightlab, 2009. All rights reserved. For Training Purposes Only Figure 1 Lift Vector Aircraft Axes X body axis “Roll axis” + right α X wind axis, Velocity Vector + up Z wind axis Y body axis “Pitch axis” + right For the aircraft below, the x-z plane (plane of symmetry) is the Z body axis surface of the paper. “Yaw axis” z x Introduction Aircraft Axes If you didn’t much care for symbols, formulas, The dashed lines in Figure 1 describe an and coefficients back in primary ground school, aircraft’s x-y-z fixed body axes, emanating from the following may raise warning signals. Ignore the center of gravity. This system, with the them and don’t be a wimp. You’ll want to mutually perpendicular axes in fixed reference to understand the axis system and also to take a the aircraft, is the one most pilots recognize. The look at the tables of aerodynamic derivatives exact alignment is a bit arbitrary. Boeing sets the (which we’ll review in person, as well). The x-axis parallel to the floorboards in its aircraft. derivatives break aircraft behavior down to cause and effect, giving the engineers lots to calculate The geometrical plane that intersects both the x and giving us the terms needed to evaluate and z body axes is called the plane of symmetry, aircraft in an informed, qualitative way—a way since a standard aircraft layout is symmetrical that links the demands of airmanship to the left and right (Figure 1, bottom).
    [Show full text]