Optimal Orbit-Raising and Attitude Control of All-Electric Satellites

Total Page:16

File Type:pdf, Size:1020Kb

Optimal Orbit-Raising and Attitude Control of All-Electric Satellites OPTIMAL ORBIT-RAISING AND ATTITUDE CONTROL OF ALL-ELECTRIC SATELLITES A Dissertation by Suwat Sreesawet Master of Science, Wichita State University, 2014 Bachelor of Engineering, Kasetsart University, 2009 Submitted to the Department of Aerospace Engineering and the faculty of the Graduate School of Wichita State University in the partial fulfillment of the requirements for the degree of Doctor of Philosophy December 2018 c Copyright 2018 by Suwat Sreesawet All Rights Reserved OPTIMAL ORBIT-RAISING AND ATTITUDE CONTROL OF ALL-ELECTRIC SATELLITES The following faculty members have examined the final copy of this dissertation for form and content, and recommend that it be accepted in partial fulfillment of the requirement for the degree of Doctor of Philosophy, with a major in Aerospace Engineering. Atri Dutta, Committee Chair James E. Steck, Committee Member Roy Myose, Committee Member Animesh Chakravarthy, Committee Member John Watkins, Committee Member Accepted for the College of Engineering Steven Skinner, Interim Dean Accepted for the Graduate School Dennis Livesay, Dean iii DEDICATION To my family, my mother, father, and sister who have always supported me and provided me the warmth to my heart for entire life, even though I am on the other side of world. To my future wife who always cares for me, and to my friends with whom I have spent many great times together. iv ACKNOWLEDGMENTS First of all, I have many thanks for my family, my dad, mon and sister. They always keep supporting and encouraging me since the day I started breathing with my own nose. I always perceive their love and support even I have been in the opposite side of the world for many years. I would like to thank my adviser, Dr. Atri Dutta, for his guidance and support all along this dissertation. He has kindly and sincerely helped since the first day i met him. I have learned a variety of knowledge from him. I would also like to thank the committee members Dr. James E. Steck, Dr. John Watkins, Dr. Animesh Chakravarthy and Dr. Roy Myose for their advice and suggestions for this research. I would like to tan I would also like to thank Ministry of Science and Technology, Thailand for funding my graduate program. I would Thanks also to my colleagues and friends who helped with their suggestions during the course of this research work. v ABSTRACT Electric propulsion is gaining popularity among satellite operators due to its fuel efficiency. However, electric propulsion has the limitation of producing a small magnitude of thrust, meaning that the transfer time to geostationary orbit is of the order of several months. The long transfer time adds more complexity to the mission design process due to the long exposure to hazardous radiation belts. Obviously, thrusters require electric power that is generated from sunlight by satellite solar panels. Therefore, the earth's shadow significantly impacts the orbit-raising maneuver. This study proposes a novel, robust, and fast numerical methodology for generating low-thrust trajectories to the geosynchronous orbit. This methodology utilizes a new set of state variables that has a physical interpretation and exhibits slow variation under a small magnitude of thrust. The absence of mathematical singularities in the equatorial plane adds to the benefits. The new set of state variables, along with a closed-loop guidance scheme and direct optimization methodology, is used to optimize the satellite trajectory. An unconstrained optimization scheme is able to robustly and rapidly generate low-thrust orbit-raising trajectories for a variety of mission scenarios, various initial orbits, application of electric battery to allow thrusting during eclipses, and orbital perturbations due to the earth's oblateness or a third body. The proposed methodology can be seamlessly integrated into receding horizon control scheme, which recomputes the minimum time trajectory at regular intervals referred to as planning horizon. The attitude of spacecraft must also be maintained in a desired direction which can be time-varying. Regular satellites perform orbit-raising using stowed solar array. In contrast, all-electric satellites perform orbit-raising using deployed solar arrays. Therefore, simple inverse controllers for attitude control with a neural network-based observer has been studied and evaluated. We demonstrate that the performance of the inverse controller is drastically improved with the proposed observer. vi TABLE OF CONTENTS Chapter Page 1. INTRODUCTION ............................... 1 1.1 Motivation . 1 1.2 Research Objective . 3 1.3 Literature Review . 4 1.3.1 Low-Thrust Orbit-Raising . 4 1.3.2 Attitude Control . 6 1.4 Contributions . 8 1.5 Organization of Dissertation . 9 2. SPACECRAFT TRANSLATIONAL DYNAMICS ............ 11 2.1 Two-Body Problem . 11 2.2 Perturbation . 14 2.2.1 Engine Thrust . 14 2.2.2 Third Body . 15 2.2.3 Earth Oblateness . 16 2.3 Set of Orbital Parameters . 17 2.3.1 Classical Orbital Elements . 17 2.3.2 Modified Equinoctial Orbital Element . 19 2.3.3 Spherical Coordinates . 21 2.4 Proposed Set of Orbital State Variables . 22 2.4.1 Reference Frames . 23 2.4.2 State Variables and Transformation . 27 2.4.3 Variation of Proposed State Variables . 30 3. SPACECRAFT ROTATIONAL DYNAMICS ............... 38 3.1 Reference Frames . 38 3.2 Attitude Representation . 39 3.2.1 Euler's Angles & Direction Cosine Matrix . 39 3.2.2 Single Rotation and Axis of Rotation . 41 3.2.3 Quaternion or Euler's Parameters . 42 3.3 Attitude Kinematics . 44 3.4 Attitude Motion . 49 4. NUMERICAL TRAJECTORY OPTIMIZATION ............. 54 4.1 Unconstrained Optimization . 54 vii TABLE OF CONTENTS (continued) Chapter Page 4.1.1 Orbit Segmentation and Eclipse Consideration . 55 4.1.2 Optimization Sub-Problem . 57 4.1.3 Terminal Conditions . 62 4.1.4 Special Case of Planar Transfer . 62 4.2 Receding Horizon Control . 64 4.2.1 Constrained Non-Linear Optimization Problem . 65 4.2.2 Initial Guess Generation . 67 5. ATTITUDE CONTROLLER DESIGN ................... 69 5.1 Inverse Controller . 69 5.2 Uncertainty and Compensation . 70 5.2.1 The Design of Modified State Observer . 72 6. SIMULATION RESULTS ........................... 79 6.1 Results of Low-Thrust Orbit-Raising . 79 6.1.1 Planar Transfers . 80 6.1.2 Non-Planar Transfers . 86 6.1.3 Sub-Optimality of Computed Solutions . 91 6.2 Receding Horizon Control . 92 6.3 Attitude Controller . 95 7. ATTITUDE CONTROL TESTBED DESIGN ............... 105 7.1 Background . 105 7.1.1 State of Spherical Air Bearing Testbed . 106 7.2 Testbed Design . 107 7.2.1 Mechanical Design . 108 7.2.2 Electrical Design . 113 8. CONCLUSIONS ................................ 126 8.1 Thesis Summary . 126 8.2 Future Work . 128 8.2.1 Low-Thrust Trajectory Generation . 128 8.2.2 Attitude Controller . 129 8.2.3 Attitude Control Testbed . 130 REFERENCES .................................... 131 viii TABLE OF CONTENTS (continued) Chapter Page Appendices ....................................... 141 ix LIST OF TABLES Table Page 3.1 List of possible rotational sequences and singularities. 39 −1 3.2 List of function S (θ2; θ3) for all Euler's angle sequence. 46 6.1 Summary of orbit-raising results. 91 6.2 Optimality gap of solutions computed using proposed methodology. 92 x LIST OF FIGURES Figure Page 1.1 Van Allen radiation belts [1]. 2 2.1 Radius vectors in two-body problem. 12 2.2 Perturbation from third body. 16 2.3 3-1-3 sequential rotation of classical orbital parameter. 18 2.4 Spherical coordinates. 22 2.5 First rotation about the basis vector J^ of frame I. 24 2.6 Second rotation about the basis vector I^0 of frame I0. 25 2.7 Third rotation about the basis vector k^ of frame O. 26 3.1 Reference frames to describe actual and desired spacecraft orientations. 38 3.2 Rotation of a reference frame about an axis. 41 3.3 Structure of spacecraft with masses. 50 3.4 Multiple-spin body. 51 4.1 Spiral shape of low-thrust trajectory (not to scale). 55 4.2 Segmentation of the trajectory over a revolution. 56 4.3 Model of the Earth's shadow. 57 4.4 Algorithm flowchart. 64 4.5 Spacecraft path planning. 65 4.6 Flowchart of receding horizon scheme. 68 5.1 Block diagram of inverse feedback control and observer. 73 5.2 Structure of neural network. 74 6.1 Result of the circular LEO to GEO transfer. 81 xi LIST OF FIGURES (continued) Figure Page 6.2 Result of GTO to GEO planar transfer. 82 6.3 Result of sub-GTO to GEO planar transfer. 83 6.4 Result of planar super-GTO to GEO planar transfer. 84 6.5 Result of circular LEO to GEO Transfer with energy storage. 85 6.6 Result of non-planar circular LEO to GEO transfer. 87 6.7 Result of the non-planar GTO to GEO Transfer. 89 6.8 Result of the non-planar LEO to GEO case with the energy storage. 90 6.9 Result of the receding horizon control in earth orbit. 94 6.10 Result of the receding horizon control in Enceladus's orbit. 95 6.11 Comparison of performance between with and without MSO. 97 6.12 Control input torque with MSO. 97 6.13 Performance of MSO . 98 6.14 Comparison of performance between the controllers with and without MSO. 100 6.15 Control input and its transient period. 101 6.16 Performance of MSO prediction . 101 6.17 Problem configuration. 102 6.18 Comparison of performance between the controllers with and without MSO. 103 6.19 Control input. 104 6.20 Performance of MSO prediction . 104 7.1 Shapes of spherical air bearing. 107 7.2 Examples of spherical attitude control testbeds. 108 xii LIST OF FIGURES (continued) Figure Page 7.3 Air bearing structure..
Recommended publications
  • Maneuver Detection of Space Object for Space Surveillance
    MANEUVER DETECTION OF SPACE OBJECT FOR SPACE SURVEILLANCE Jian Huang*, Weidong Hu, Lefeng Zhang $756WDWH.H\/DE1DWLRQDO8QLYHUVLW\RI'HIHQVH7HFKQRORJ\&KDQJVKD+XQDQ3URYLQFH&KLQD (PDLOKXDQJMLDQ#QXGWHGXFQ ABSTRACT on the technique of a moving window curve fit. Holzinger & Scheeres presented an object correlation Maneuver detection is a very important task for and maneuver detection method using optimal control maintaining the catalog of the orbital objects and space performance metrics [5]. Kelecy & Jah focused on the situational awareness. This paper mainly focuses on the detection and reconstruction of single low thrust in- typical maneuver scenario where space objects only track maneuvers by using the orbit determination perform tangential orbital maneuvers during a relative strategies based on the batch least-squares and long gap. Particularly, only two classical and extended Kalman filter (EKF) [6]. However, these commonly applied orbital transition manners are methods are highly relevant to the presupposed considered, i.e. the twice tangential maneuvers at the maneuvering mode and a relative short observation gap. apogee and the perigee or one tangential maneuver at In this paper, to address the real observed data, we only an arbitrary time. Based on this, we preliminarily consider the common maneuvering modes and estimate the maneuvering mode and parameters by observation scenarios in practical. For an orbital analyzing the change of semi-major axis and maneuver, minimization of fuel consumption is eccentricity. Furthermore, if only one tangential essential because the weight of a payload that can be maneuver happened, we can formulate the estimation carried to the desired orbit depends on this problem of maneuvering parameters as a non-linear minimization.
    [Show full text]
  • Reduction of Saturn Orbit Insertion Impulse Using Deep-Space Low Thrust
    Reduction of Saturn Orbit Insertion Impulse using Deep-Space Low Thrust Elena Fantino ∗† Khalifa University of Science and Technology, Abu Dhabi, United Arab Emirates. Roberto Flores‡ International Center for Numerical Methods in Engineering, 08034 Barcelona, Spain. Jesús Peláez§ and Virginia Raposo-Pulido¶ Technical University of Madrid, 28040 Madrid, Spain. Orbit insertion at Saturn requires a large impulsive manoeuver due to the velocity difference between the spacecraft and the planet. This paper presents a strategy to reduce dramatically the hyperbolic excess speed at Saturn by means of deep-space electric propulsion. The inter- planetary trajectory includes a gravity assist at Jupiter, combined with low-thrust maneuvers. The thrust arc from Earth to Jupiter lowers the launch energy requirement, while an ad hoc steering law applied after the Jupiter flyby reduces the hyperbolic excess speed upon arrival at Saturn. This lowers the orbit insertion impulse to the point where capture is possible even with a gravity assist with Titan. The control-law algorithm, the benefits to the mass budget and the main technological aspects are presented and discussed. The simple steering law is compared with a trajectory optimizer to evaluate the quality of the results and possibilities for improvement. I. Introduction he giant planets have a special place in our quest for learning about the origins of our planetary system and Tour search for life, and robotic missions are essential tools for this scientific goal. Missions to the outer planets arXiv:2001.04357v1 [astro-ph.EP] 8 Jan 2020 have been prioritized by NASA and ESA, and this has resulted in important space projects for the exploration of the Jupiter system (NASA’s Europa Clipper [1] and ESA’s Jupiter Icy Moons Explorer [2]), and studies are underway to launch a follow-up of Cassini/Huygens called Titan Saturn System Mission (TSSM) [3], a joint ESA-NASA project.
    [Show full text]
  • Telecommunikation Satellites: the Actual Situation and Potential Future Developments
    Telecommunikation Satellites: The Actual Situation and Potential Future Developments Dr. Manfred Wittig Head of Multimedia Systems Section D-APP/TSM ESTEC NL 2200 AG Noordwijk [email protected] March 2003 Commercial Satellite Contracts 25 20 15 Europe US 10 5 0 1995 1996 1997 1998 1999 2000 2001 2002 2003 European Average 5 Satellites/Year US Average 18 Satellites/Year Estimation of cumulative value chain for the Global commercial market 1998-2007 in BEuro 35 27 100% 135 90% 80% 225 Spacecraft Manufacturing 70% Launch 60% Operations Ground Segment 50% Services 40% 365 30% 20% 10% 0% 1 Consolidated Turnover of European Industry Commercial Telecom Satellite Orders 2000 30 2001 25 2002 3 (7) Firm Commercial Telecom Satellite Orders in 2002 Manufacturer Customer Satellite Astrium Hispasat SA Amazonas (Spain) Boeing Thuraya Satellite Thuraya 3 Telecommunications Co (U.A.E.) Orbital Science PT Telekommunikasi Telkom-2 Indonesia Hangar Queens or White Tails Orders in 2002 for Bargain Prices of already contracted Satellites Manufacturer Customer Satellite Alcatel Space New Indian Operator Agrani (India) Alcatel Space Eutelsat W5 (France) (1998 completed) Astrium Hellas-Sat Hellas Sat Consortium Ltd. (Greece-Cyprus) Commercial Telecom Satellite Orders in 2003 Manufacturer Customer Satellite Astrium Telesat Anik F1R 4.2.2003 (Canada) Planned Commercial Telecom Satellite Orders in 2003 SES GLOBAL Three RFQ’s: SES Americom ASTRA 1L ASTRA 1K cancelled four orders with Alcatel Space in 2001 INTELSAT Launched five satellites in the last 13 month average fleet age: 11 Years of remaining life PanAmSat No orders expected Concentration on cash flow generation Eutelsat HB 7A HB 8 expected at the end of 2003 Telesat Ordered Anik F1R from Astrium Planned Commercial Telecom Satellite Orders in 2003 Arabsat & are expected to replace Spacebus 300 Shin Satellite (solar-array steering problems) Korea Telecom Negotiation with Alcatel Space for Koreasat Binariang Sat.
    [Show full text]
  • Analysis of Transfer Maneuvers from Initial
    Revista Mexicana de Astronom´ıa y Astrof´ısica, 52, 283–295 (2016) ANALYSIS OF TRANSFER MANEUVERS FROM INITIAL CIRCULAR ORBIT TO A FINAL CIRCULAR OR ELLIPTIC ORBIT M. A. Sharaf1 and A. S. Saad2,3 Received March 14 2016; accepted May 16 2016 RESUMEN Presentamos un an´alisis de las maniobras de transferencia de una ´orbita circu- lar a una ´orbita final el´ıptica o circular. Desarrollamos este an´alisis para estudiar el problema de las transferencias impulsivas en las misiones espaciales. Consideramos maniobras planas usando ecuaciones reci´enobtenidas; con estas ecuaciones se com- paran las maniobras circulares y el´ıpticas. Esta comparaci´on es importante para el dise˜no´optimo de misiones espaciales, y permite obtener mapeos ´utiles para mostrar cu´al es la mejor maniobra. Al respecto, desarrollamos este tipo de comparaciones mediante 10 resultados, y los mostramos gr´aficamente. ABSTRACT In the present paper an analysis of the transfer maneuvers from initial circu- lar orbit to a final circular or elliptic orbit was developed to study the problem of impulsive transfers for space missions. It considers planar maneuvers using newly derived equations. With these equations, comparisons of circular and elliptic ma- neuvers are made. This comparison is important for the mission designers to obtain useful mappings showing where one maneuver is better than the other. In this as- pect, we developed this comparison throughout ten results, together with some graphs to show their meaning. Key Words: celestial mechanics — methods: analytical — space vehicles 1. INTRODUCTION The large amount of information from interplanetary missions, such as Pioneer (Dyer et al.
    [Show full text]
  • ORBIT MANOUVERS • Orbital Plane Change (Inclination) It Is an Orbital
    UNIVERSITY OF ANBAR ADVANCED COMMUNICATIONS SYSTEMS FOR 4th CLASS STUDENTS COLLEGE OF ENGINEERING by: Dr. Naser Al-Falahy ELECTRICAL ENGINEERING WE EK 4 ORBIT MANOUVERS Orbital plane change (inclination) It is an orbital maneuver aimed at changing the inclination of an orbiting body's orbit. This maneuver is also known as an orbital plane change as the plane of the orbit is tipped. This maneuver requires a change in the orbital velocity vector (delta v) at the orbital nodes (i.e. the point where the initial and desired orbits intersect, the line of orbital nodes is defined by the intersection of the two orbital planes). In general, inclination changes can take a very large amount of delta v to perform, and most mission planners try to avoid them whenever possible to conserve fuel. This is typically achieved by launching a spacecraft directly into the desired inclination, or as close to it as possible so as to minimize any inclination change required over the duration of the spacecraft life. When both orbits are circular (i.e. e = 0) and have the same radius the Delta-v (Δvi) required for an inclination change (Δvi) can be calculated using: where: v is the orbital velocity and has the same units as Δvi (Δi ) inclination change required. Example Calculate the velocity change required to transfer a satellite from a circular 600 km orbit with an inclination of 28 degrees to an orbit of equal size with an inclination of 20 degrees. SOLUTION, r = (6,378.14 + 600) × 1,000 = 6,978,140 m , ϑ = 28 - 20 = 8 degrees Vi = SQRT[ GM / r ] Vi = SQRT[ 3.986005×1014 / 6,978,140 ] Vi = 7,558 m/s Δvi = 2 × Vi × sin(ϑ/2) Δvi = 2 × 7,558 × sin(8/2) Δvi = 1,054 m/s 18 UNIVERSITY OF ANBAR ADVANCED COMMUNICATIONS SYSTEMS FOR 4th CLASS STUDENTS COLLEGE OF ENGINEERING by: Dr.
    [Show full text]
  • Boeing 702 Fleet
    Boeing 702 Fleet ! List of Boeing 702 Satellite operators have Programs responded enthusiastically to the vastly increased ! List of 702s On Order capabilities represented by the Boeing 702. Boeing Satellite Systems (BSS) announced the innovative satellite series in October 1995. Evolved from the popular, proven 601 and 601HP (high-power) spacecraft, the body- stabilized Boeing 702 is the 01PR 01507 world leader in capacity, High resolution image available here performance and cost- efficiency. As of June 2005, 19 of these powerful satellites had been ordered, with options for six more. The first satellite was launched in 1999. The satellite can carry more than 100 high-power transponders, and deliver any communications frequencies that customers request. The Boeing 702 design is directly responsive to what customers said they wanted in a communications satellite, beginning with lower cost and including the high reliability for which the company is renowned. For maximum customer value and producibility at minimum total cost, the Boeing 702 offers a broad spectrum of modularity. A primary example is payload/bus integration. After the payload is tailored to customer specifications, the payload module mounts to the common bus module at only four locations and with only six electrical connectors. This design simplicity confers major advantages. First, nonrecurring program costs are reduced, because the bus does not need to be changed for every payload, and payloads can be freely tailored without affecting the bus. Second, the design permits significantly faster parallel bus and payload processing. This leads to the third advantage: a short production schedule. Further efficiency derives from the 702's advanced xenon ion propulsion system (XIPS), which was pioneered by BSS and is produced today by Boeing Electron Dynamic Devices, Inc.
    [Show full text]
  • Collision Probability Prediction and Orbit Maneuvering Probability Determination of Non-Cooperative Space Object Orbit
    remote sensing Article Collision Probability Prediction and Orbit Maneuvering Probability Determination of Non-Cooperative Space Object Orbit 1,2 3 1, 1 1, , Yuanlan Wen , Zhuo Yu , Lina He y, Qian Wang and Xiufeng He * y 1 School of Earth Science and Engineering, Hohai University, Nanjing 210098, China; [email protected] (Y.W.); [email protected] (L.H.); [email protected] (Q.W.) 2 Research School of High Technology, Hunan Institute of Traffic Engineering, Hengyang 421099, China 3 Xi’an Satellite Control Center, Xi’an 710043, China; [email protected] * Correspondence: [email protected] These authors contributed equally to the work. y Received: 5 September 2020; Accepted: 1 October 2020; Published: 12 October 2020 Abstract: Probability of collision between non-cooperative space object (NCSO) and the reference spacecraft (RS) has been increased drastically over the past few decades. The traditional method is difficult to identify the maneuvering of non-cooperative space object. In the present paper, not only positions and velocities, but also accelerations of non-cooperative space object are estimated as parameters by the extended Kalman filtering based on setting up the state linear equation and measurement model of the non-cooperative space object. The algorithm for predicting collision probability is derived from position error ellipsoid, and the algorithm for determining maneuvering probability is derived from maneuvering acceleration and its error ellipsoid, which can be employed to identify whether the upcoming space object is being maneuvered. An epoch Earth-centered inertial (EECI) coordinate system is suggested to replace Earth-centered inertial (ECI) to simplify coordinate transformation.
    [Show full text]
  • Orbital Mechanics Course Notes
    Orbital Mechanics Course Notes David J. Westpfahl Professor of Astrophysics, New Mexico Institute of Mining and Technology March 31, 2011 2 These are notes for a course in orbital mechanics catalogued as Aerospace Engineering 313 at New Mexico Tech and Aerospace Engineering 362 at New Mexico State University. This course uses the text “Fundamentals of Astrodynamics” by R.R. Bate, D. D. Muller, and J. E. White, published by Dover Publications, New York, copyright 1971. The notes do not follow the book exclusively. Additional material is included when I believe that it is needed for clarity, understanding, historical perspective, or personal whim. We will cover the material recommended by the authors for a one-semester course: all of Chapter 1, sections 2.1 to 2.7 and 2.13 to 2.15 of Chapter 2, all of Chapter 3, sections 4.1 to 4.5 of Chapter 4, and as much of Chapters 6, 7, and 8 as time allows. Purpose The purpose of this course is to provide an introduction to orbital me- chanics. Students who complete the course successfully will be prepared to participate in basic space mission planning. By basic mission planning I mean the planning done with closed-form calculations and a calculator. Stu- dents will have to master additional material on numerical orbit calculation before they will be able to participate in detailed mission planning. There is a lot of unfamiliar material to be mastered in this course. This is one field of human endeavor where engineering meets astronomy and ce- lestial mechanics, two fields not usually included in an engineering curricu- lum.
    [Show full text]
  • Innovative Commercial Satellite Approaches for Space Related Ground Systems
    Ground Systems Architecture Workshop 2014 Mobility Briefing Innovative Commercial Satellite Approaches for Space Related Ground Systems February• August 26, 2011 2014 Mark Daniels VP Engineering and Operations Intelsat General Corporation © 2014 by Intelsat General Corporation. Published by The Aerospace Corporation with permission Proprietary & Confidential 1 General Shelton Quote On January 7, 2014 In Response To Question About Commercial Industry’s Role In Military Space: “ Why couldn’t we contract for all standard wideband communication services? “Why couldn’t that be written by commercial providers instead of us buying our own satellites?” June 28, 2010 The U.S. government will use commercial space products and services in fulfilling governmental needs, invest in new and advanced technologies and concepts, and use a broad array of partnerships with industry to promote innovation. 2 SM 50+ satellites in geostationary orbit IntelsatOne 40,000 miles of MPLS terrestrial infrastructure Global presence, global footprint 3 Intelsat Satellite Operations Experience Currently 76 Satellites Operated (51 Intelsat and 25 Third Party) 14 Bus platforms Astrium E2000 Astrium E3000 Boeing 381 Boeing 393 Boeing 601 Boeing 601HP Boeing 601MEO Boeing 702 Boeing 702MP LM 7000 OSC Star 2 SSL 1300 Omega SSL FS1300 Thales Spacebus 3000B 4 Satellite Operations • Fully redundant primary and back up control centers in Washington, DC and Long Beach, CA • Operational experience with all major manufacturers and satellite platforms • Highly functional and automated
    [Show full text]
  • Last Class Commercial C Rew S a N D Private Astronauts Will Boost International S P a C E • Where Do Objects Get Their Energy?
    9/9/2020 Today’s Class: Gravity & Spacecraft Trajectories CU Astronomy Club • Read about Explorer 1 at • Need some Space? http://en.wikipedia.org/wiki/Explorer_1 • Read about Van Allen Radiation Belts at • Escape the light pollution, join us on our Dark Sky http://en.wikipedia.org/wiki/Van_Allen_radiation_belt Trips • Complete Daily Health Form – Stargazing, astrophotography, and just hanging out – First trip: September 11 • Open to all majors! • The stars respect social distancing and so do we • Head to our website to join our email list: https://www.colorado.edu/aps/our- department/outreach/cu-astronomy-club • Email Address: [email protected] Astronomy 2020 – Space Astronomy & Exploration Astronomy 2020 – Space Astronomy & Exploration 1 2 Last Class Commercial C rew s a n d Private Astronauts will boost International S p a c e • Where do objects get their energy? Article by Elizabeth Howell Station's Sci enc e Presentation by Henry Universe Today/SpaceX –Conservation of energy: energy Larson cannot be created or destroyed but ● SpaceX’s Demo 2 flight showed what human spaceflight Question: can look like under private enterprise only transformed from one type to ● NASArelied on Russia’s Soyuz spacecraft to send astronauts to the ISS in the past another. ● "We're going to have more people on the International Space Station than we've had in a long time,” NASA –Energy comes in three basic types: Administrator Jim Bridenstine ● NASAis primarily using SpaceX and Boeing for their kinetic, potential, radiative. “commercial crew”program Astronomy 2020 – Space Astronomy & Exploration 3 4 Class Exercise: Which of the following Today’s Learning Goals processes violates a conservation law? • What are range of common Earth a) Mass is converted directly into energy.
    [Show full text]
  • Fundamentals of Orbital Mechanics
    Chapter 7 Fundamentals of Orbital Mechanics Celestial mechanics began as the study of the motions of natural celestial bodies, such as the moon and planets. The field has been under study for more than 400 years and is documented in great detail. A major study of the Earth-Moon-Sun system, for example, undertaken by Charles-Eugene Delaunay and published in 1860 and 1867 occupied two volumes of 900 pages each. There are textbooks and journals that treat every imaginable aspect of the field in abundance. Orbital mechanics is a more modern treatment of celestial mechanics to include the study the motions of artificial satellites and other space vehicles moving un- der the influences of gravity, motor thrusts, atmospheric drag, solar winds, and any other effects that may be present. The engineering applications of this field include launch ascent trajectories, reentry and landing, rendezvous computations, orbital design, and lunar and planetary trajectories. The basic principles are grounded in rather simple physical laws. The paths of spacecraft and other objects in the solar system are essentially governed by New- ton’s laws, but are perturbed by the effects of general relativity (GR). These per- turbations may seem relatively small to the layman, but can have sizable effects on metric predictions, such as the two-way round trip Doppler. The implementa- tion of post-Newtonian theories of orbital mechanics is therefore required in or- der to meet the accuracy specifications of MPG applic ations. Because it had the need for very accurate trajectories of spacecraft, moon, and planets, dating back to the 1950s, JPL organized an effort that soon became the world leader in the field of orbital mechanics and space navigation.
    [Show full text]
  • Ad-Hoc Regional Coverage Constellations of Cubesats Using Secondary Launches
    AD-HOC REGIONAL COVERAGE CONSTELLATIONS OF CUBESATS USING SECONDARY LAUNCHES A Thesis Presented to the Faculty of California Polytechnic State University, San Luis Obispo In Partial Fulfillment of the Requirements for the Degree Master of Science in Aerospace Engineering by Guy G. Zohar March 2013 © 2013 Guy G. Zohar ALL RIGHTS RESERVED ii COMMITTEE MEMBERSHIP TITLE: Ad-Hoc Regional Coverage Constellations of CubeSats using Secondary Launches AUTHOR: Guy G. Zohar DATE SUBMITTED: March 2013 COMMITTEE CHAIR: Dr. Jordi Puig-Suari, Professor Cal Poly Aerospace Engineering Department COMMITTEE MEMBER: Dr. Kira J Abercromby, Assistant Professor Cal Poly Aerospace Engineering Department COMMITTEE MEMBER: Daniel J Wait; Lecturer Cal Poly Aerospace Engineering Department COMMITTEE MEMBER: Dr. Gerald L. Shaw; Senior Research Engineer SRI International iii ABSTRACT Ad-Hoc Regional Coverage Constellations of CubeSats Using Secondary Launches Guy G. Zohar As development of CubeSat based architectures increase, methods of deploying constellations of CubeSats are required to increase functionality of future systems. Given their low cost and quickly increasing launch opportunities, large numbers of CubeSats can easily be developed and deployed in orbit. However, as secondary payloads, CubeSats are severely limited in their options for deployment into appropriate constellation geometries. This thesis examines the current methods for deploying cubes and proposes new and efficient geometries using secondary launch opportunities. Due to the current deployment hardware architecture, only the use of different launch opportunities, deployment direction, and deployment timing for individual cubes in a single launch are explored. The deployed constellations are examined for equal separation of Cubes in a single plane and effectiveness of ground coverage of two regions.
    [Show full text]