Trajectory Sensitivities for Sun-Mars Libration Point Missions
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Astrodynamics
Politecnico di Torino SEEDS SpacE Exploration and Development Systems Astrodynamics II Edition 2006 - 07 - Ver. 2.0.1 Author: Guido Colasurdo Dipartimento di Energetica Teacher: Giulio Avanzini Dipartimento di Ingegneria Aeronautica e Spaziale e-mail: [email protected] Contents 1 Two–Body Orbital Mechanics 1 1.1 BirthofAstrodynamics: Kepler’sLaws. ......... 1 1.2 Newton’sLawsofMotion ............................ ... 2 1.3 Newton’s Law of Universal Gravitation . ......... 3 1.4 The n–BodyProblem ................................. 4 1.5 Equation of Motion in the Two-Body Problem . ....... 5 1.6 PotentialEnergy ................................. ... 6 1.7 ConstantsoftheMotion . .. .. .. .. .. .. .. .. .... 7 1.8 TrajectoryEquation .............................. .... 8 1.9 ConicSections ................................... 8 1.10 Relating Energy and Semi-major Axis . ........ 9 2 Two-Dimensional Analysis of Motion 11 2.1 ReferenceFrames................................. 11 2.2 Velocity and acceleration components . ......... 12 2.3 First-Order Scalar Equations of Motion . ......... 12 2.4 PerifocalReferenceFrame . ...... 13 2.5 FlightPathAngle ................................. 14 2.6 EllipticalOrbits................................ ..... 15 2.6.1 Geometry of an Elliptical Orbit . ..... 15 2.6.2 Period of an Elliptical Orbit . ..... 16 2.7 Time–of–Flight on the Elliptical Orbit . .......... 16 2.8 Extensiontohyperbolaandparabola. ........ 18 2.9 Circular and Escape Velocity, Hyperbolic Excess Speed . .............. 18 2.10 CosmicVelocities -
AAS/AIAA Astrodynamics Specialist Conference
DRAFT version: 7/15/2011 11:04 AM http://www.alyeskaresort.com AAS/AIAA Astrodynamics Specialist Conference July 31 ‐ August 4, 2011 Girdwood, Alaska AAS General Chair AIAA General Chair Ryan P. Russell William Todd Cerven Georgia Institute of Technology The Aerospace Corporation AAS Technical Chair AIAA Technical Chair Hanspeter Schaub Brian C. Gunter University of Colorado Delft University of Technology DRAFT version: 7/15/2011 11:04 AM http://www.alyeskaresort.com Cover images: Top right: Conference Location: Aleyska Resort in Girdwood Alaska. Middle left: Cassini looking back at an eclipsed Saturn, Astronomy picture of the day 2006 Oct 16, credit CICLOPS, JPL, ESA, NASA; Middle right: Shuttle shadow in the sunset (in honor of the end of the Shuttle Era), Astronomy picture of the day 2010 February 16, credit: Expedition 22 Crew, NASA. Bottom right: Comet Hartley 2 Flyby, Astronomy picture of the day 2010 Nov 5, Credit: NASA, JPL-Caltech, UMD, EPOXI Mission DRAFT version: 7/15/2011 11:04 AM http://www.alyeskaresort.com Table of Contents Registration ............................................................................................................................................... 5 Schedule of Events ................................................................................................................................... 6 Conference Center Layout ........................................................................................................................ 7 Conference Location: The Hotel Alyeska ............................................................................................... -
Aas 11-509 Artemis Lunar Orbit Insertion and Science Orbit Design Through 2013
AAS 11-509 ARTEMIS LUNAR ORBIT INSERTION AND SCIENCE ORBIT DESIGN THROUGH 2013 Stephen B. Broschart,∗ Theodore H. Sweetser,y Vassilis Angelopoulos,z David C. Folta,x and Mark A. Woodard{ As of late-July 2011, the ARTEMIS mission is transferring two spacecraft from Lissajous orbits around Earth-Moon Lagrange Point #1 into highly-eccentric lunar science orbits. This paper presents the trajectory design for the transfer from Lissajous orbit to lunar orbit in- sertion, the period reduction maneuvers, and the science orbits through 2013. The design accommodates large perturbations from Earth’s gravity and restrictive spacecraft capabili- ties to enable opportunities for a range of heliophysics and planetary science measurements. The process used to design the highly-eccentric ARTEMIS science orbits is outlined. The approach may inform the design of future eccentric orbiter missions at planetary moons. INTRODUCTION The Acceleration, Reconnection, Turbulence and Electrodynamics of the Moons Interaction with the Sun (ARTEMIS) mission is currently operating two spacecraft in lunar orbit under funding from the Heliophysics and Planetary Science Divisions with NASA’s Science Missions Directorate. ARTEMIS is an extension to the successful Time History of Events and Macroscale Interactions during Substorms (THEMIS) mission [1] that has relocated two of the THEMIS spacecraft from Earth orbit to the Moon [2, 3, 4]. ARTEMIS plans to conduct a variety of scientific studies at the Moon using the on-board particle and fields instrument package [5, 6]. The final portion of the ARTEMIS transfers involves moving the two ARTEMIS spacecraft, known as P1 and P2, from Lissajous orbits around the Earth-Moon Lagrange Point #1 (EML1) to long-lived, eccentric lunar science orbits with periods of roughly 28 hr. -
Rare Astronomical Sights and Sounds
Jonathan Powell Rare Astronomical Sights and Sounds The Patrick Moore The Patrick Moore Practical Astronomy Series More information about this series at http://www.springer.com/series/3192 Rare Astronomical Sights and Sounds Jonathan Powell Jonathan Powell Ebbw Vale, United Kingdom ISSN 1431-9756 ISSN 2197-6562 (electronic) The Patrick Moore Practical Astronomy Series ISBN 978-3-319-97700-3 ISBN 978-3-319-97701-0 (eBook) https://doi.org/10.1007/978-3-319-97701-0 Library of Congress Control Number: 2018953700 © Springer Nature Switzerland AG 2018 This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilms or in any other physical way, and transmission or information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed. The use of general descriptive names, registered names, trademarks, service marks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. The publisher, the authors, and the editors are safe to assume that the advice and information in this book are believed to be true and accurate at the date of publication. Neither the publisher nor the authors or the editors give a warranty, express or implied, with respect to the material contained herein or for any errors or omissions that may have been made. -
Applications of Multi-Body Dynamical Environments: the ARTEMIS Transfer Trajectory Design
Paper ID: 7461 61st International Astronautical Congress 2010 Applications of Multi-Body Dynamical Environments: The ARTEMIS Transfer Trajectory Design ASTRODYNAMICS SYMPOSIUM (CI) Mission Design, Operations and Optimization (2) (9) Mr. David C. Folta and Mr. Mark Woodard National Aeronautics and Space Administration (NASA)/Goddard Space Flight Center, Greenbelt, MD, United States, david.c.folta<@nasa.gov Prof. Kathleen Howell, Chris Patterson, Wayne Schlei Purdue University, West Lafayette, IN, United States, [email protected] Abstract The application of forces in multi-body dynamical environments to pennit the transfer of spacecraft from Earth orbit to Sun-Earth weak stability regions and then return to the Earth-Moon libration (L1 and L2) orbits has been successfully accomplished for the first time. This demonstrated transfer is a positive step in the realization of a design process that can be used to transfer spacecraft with minimal Delta-V expenditures. Initialized using gravity assists to overcome fuel constraints; the ARTEMIS trajectory design has successfully placed two spacecraft into Earth Moon libration orbits by means of these applications. INTRODUCTION The exploitation of multi-body dynamical environments to pennit the transfer of spacecraft from Earth to Sun-Earth weak stability regions and then return to the Earth-Moon libration (L 1 and L2) orbits has been successfully accomplished. This demonstrated transfer is a positive step in the realization of a design process that can be used to transfer spacecraft with minimal Delta-Velocity (L.\V) expenditure. Initialized using gravity assists to overcome fuel constraints, the Acceleration Reconnection and Turbulence and Electrodynamics of the Moon's Interaction with the Sun (ARTEMIS) mission design has successfully placed two spacecraft into Earth-Moon libration orbits by means of this application of forces from multiple gravity fields. -
Libration Orbit Mission Design: Applications of Numerical and Dynamical Methods
Libration Orbit Mission Design: Applications Of Numerical And Dynamical Methods David Folta and Mark Beckman NASA - Goddard Space Flight Center Libration Point Orbits and Applications June 10-14, 2002, Girona, Spain Agenda • NASA Enterprises • Challenges • Historical and future missions • Libration mission design via numerical and dynamical methods • Applications ¾Direct transfer ¾Low thrust ¾Servicing ¾Formations: Constellation-X and Stellar Imager ¾Conceptual studies • Improved tools • Conclusions NASA Themes and Libration Orbits NASA Enterprises of Space Sciences (SSE) and Earth Sciences (ESE) are a combination of several programs and themes SSE ESE SEU SEC Origins • Recent SEC missions include ACE, SOHO, and the L1/L2 WIND mission. The Living With a Star (LWS) portion of SEC may require libration orbits at the L1 and L3 Sun-Earth libration points. • Structure and Evolution of the Universe (SEU) currently has MAP and the future Micro Arc-second X-ray Imaging Mission (MAXIM) and Constellation-X missions. •Space Sciences’ Origins libration missions are the Next Generation Space Telescope (NGST) and The Terrestrial Planet Finder (TPF). • The Triana mission is the lone ESE mission not orbiting the Earth. • A major challenge is formation flying components of Constellation-X, MAXIM, TPF, and Stellar Imager. Future Libration Mission SSE and ESE Challenges ¾ Orbit ¾Biased orbits when using large sun shades ¾Shadow restrictions ¾Very small amplitudes ¾Reorientation to different planes and Lissajous classes ¾Rendezvous and formation flying ¾Low -
Tellurium Tellurium N
Experiment Description/Manual Tellurium Tellurium N Table of contents General remarks ............................................................................................................................3 Important parts of the Tellurium and their operation .....................................................................4 Teaching units for working with the Tellurium: Introduction: From one´s own shadow to the shadow-figure on the globe of the Tellurium ...........6 1. The earth, a gyroscope in space ............................................................................................8 2. Day and night ..................................................................................................................... 10 3. Midday line and division of hours ....................................................................................... 13 4. Polar day and polar night .................................................................................................... 16 5. The Tropic of Cancer and Capricorn and the tropics ........................................................... 17 6. The seasons ........................................................................................................................ 19 7. Lengths of day and night in various latitudes ......................................................................22 Working sheet “Lengths of day in various seasons” ............................................................ 24 8. The times of day .................................................................................................................25 -
Stationkeeping in and Design of Transfer Between Earth-Moon L1,2 Orbits: ARTEMIS Mission Results
Goddard Space Flight Center Stationkeeping in and Design of Transfer Between Earth-Moon L1,2 Orbits: ARTEMIS Mission Results Future In-Space Operations (FISO) Dave Folta Goddard Space Flight Center February, 23, 2011 Agenda Goddard Space Flight Center • General Libration Orbit Background • Stationkeeping Methods • The ARTEMIS Mission Results and Operations • Stationkeeping Observations • Comparison to Other Lunar Orbits • Summary Libration Orbit Dynamics Goddard Space Flight Center Where Are They? What Are They?? Collinear Points: L1, L2, L3 (unstable) Equilibrium or libration points represent Triangular Points: L4, L5 (stable) singularities in the equations of motion where velocity and acceleration components are zero and the forces are balanced Viewed in the rotating frame: centrifugal L4 (Coriolis-Type) force balances with gravitational forces of the two primaries 1 a.u. 1 a.u. Libration points are in plane with no Z component. Orbits are mapped to a rotating L3 Sun L1 L2 frame where there are no time dependent forces 0.01 a.u. A system of interest involves the Sun (m1), Earth/Moon System the Earth-Moon system (m2) and the spacecraft m3 L1 and L2 At a distance of 1.5 million km L5 L4 and L5 At a distance of 150. million km Solar Rotating Coordinates Ecliptic Plane Projection Rotating Coordinate Frames Goddard Space Flight Center Sun-Earth & Earth-Moon • X is towards smaller body (sun to Earth) • Y is along smaller body velocity • Z is out of Ecliptic plane • Co-linear Unstable locations at L1, L2, and ‘L3’ • Stable locations -
SERVICING and DEPLOYMENT of NATIONAL RESOURCES in SUN-EARTH LIBRATION POINT ORBITS 53Th International Astronautical Congress
SERVICING AND DEPLOYMENT OF NATIONAL RESOURCES IN SUN-EARTH LIBRATION POINT ORBITS D. C. Folta, M. Beckman, S. J. Leete, G. C. Marr, M. Mesarch, and S. Cooley NASA Goddard Space Flight Center Greenbelt, MD, USA 53th International Astronautical Congress The World Space Congress - 2002 10-3 9 Oct 2002 I Houston, Texas For permission to copy or republish, contact the International Astronautical Federation, 3-5 Rue Mario-Nikis, 75015 Paris, France SERVICING AND DEPLOYMENT OF NATIONAL RESOURCES IN SUN-EARTH LIBRATION POINT ORBITS D. C. Folta, M. Beckman, G. C. Marr, M. Mesarch, S. Cooley Flight Dynamics Analysis Branch NASA Goddard Space Flight Center, Greenbelt, MD, USA dfolta@;gsfc.nasa.gov S. J. Leete Space Science Missions Branch, NASA Goddard Space Flight Center, Greenbelt, MD, USA Abstract Spacecraft travel between the Sun-Earth system, the Earth-Moon system, and beyond has received extensive attention recently. The existence of a connection between unstable regions enables mission designers to envision scenarios of multiple spacecraft traveling cheaply from system to system, rendezvousing, servicing, and refbeling along the way. This paper presents examples of transfers between the Sun-Earth and Earth-Moon systems using a true ephemeris and perturbation model. It shows the AV costs associated with these transfers, including the costs to reach the staging region from the Earth. It explores both impulsive and low thrust transfer trajectories. Additionally, analysis that looks specifically at the use of nuclear power in libration point orbits and the issues associated with them such as inadvertent Earth return is addressed. Statistical analysis of Earth returns and the design of biased orbits to prevent any possible return are discussed. -
Lunar Laser Ranging: the Millimeter Challenge
REVIEW ARTICLE Lunar Laser Ranging: The Millimeter Challenge T. W. Murphy, Jr. Center for Astrophysics and Space Sciences, University of California, San Diego, 9500 Gilman Drive, La Jolla, CA 92093-0424, USA E-mail: [email protected] Abstract. Lunar laser ranging has provided many of the best tests of gravitation since the first Apollo astronauts landed on the Moon. The march to higher precision continues to this day, now entering the millimeter regime, and promising continued improvement in scientific results. This review introduces key aspects of the technique, details the motivations, observables, and results for a variety of science objectives, summarizes the current state of the art, highlights new developments in the field, describes the modeling challenges, and looks to the future of the enterprise. PACS numbers: 95.30.Sf, 04.80.-y, 04.80.Cc, 91.4g.Bg arXiv:1309.6294v1 [gr-qc] 24 Sep 2013 CONTENTS 2 Contents 1 The LLR concept 3 1.1 Current Science Results . 4 1.2 A Quantitative Introduction . 5 1.3 Reflectors and Divergence-Imposed Requirements . 5 1.4 Fundamental Measurement and World Lines . 10 2 Science from LLR 12 2.1 Relativity and Gravity . 12 2.1.1 Equivalence Principle . 13 2.1.2 Time-rate-of-change of G ....................... 14 2.1.3 Gravitomagnetism, Geodetic Precession, and other PPN Tests . 14 2.1.4 Inverse Square Law, Extra Dimensions, and other Frontiers . 16 2.2 Lunar and Earth Physics . 16 2.2.1 The Lunar Interior . 16 2.2.2 Earth Orientation, Precession, and Coordinate Frames . 18 3 LLR Capability across Time 20 3.1 Brief LLR History . -
Moon-Earth-Sun: the Oldest Three-Body Problem
Moon-Earth-Sun: The oldest three-body problem Martin C. Gutzwiller IBM Research Center, Yorktown Heights, New York 10598 The daily motion of the Moon through the sky has many unusual features that a careful observer can discover without the help of instruments. The three different frequencies for the three degrees of freedom have been known very accurately for 3000 years, and the geometric explanation of the Greek astronomers was basically correct. Whereas Kepler’s laws are sufficient for describing the motion of the planets around the Sun, even the most obvious facts about the lunar motion cannot be understood without the gravitational attraction of both the Earth and the Sun. Newton discussed this problem at great length, and with mixed success; it was the only testing ground for his Universal Gravitation. This background for today’s many-body theory is discussed in some detail because all the guiding principles for our understanding can be traced to the earliest developments of astronomy. They are the oldest results of scientific inquiry, and they were the first ones to be confirmed by the great physicist-mathematicians of the 18th century. By a variety of methods, Laplace was able to claim complete agreement of celestial mechanics with the astronomical observations. Lagrange initiated a new trend wherein the mathematical problems of mechanics could all be solved by the same uniform process; canonical transformations eventually won the field. They were used for the first time on a large scale by Delaunay to find the ultimate solution of the lunar problem by perturbing the solution of the two-body Earth-Moon problem. -
Analysis of the Gaia Orbit Around L2
TREBALL DE FI DE CARRERA TÍTOL DEL TFC: Analysis of the Gaia orbit around L2 TITULACIÓ: Enginyeria Tècnica Aeronàutica, especialitat Aeronavegació AUTOR: Jordi Carlos García García DIRECTORS: Santiago Torres Gil, Enrique García-Berro Montilla 2 Analysis of the Gaia orbit around L2 DATA: 27 de juliol de 2009 Títol: Analysis of the Gaia orbit around L2 Autor: Jordi Carlos García García Directors: Santiago Torres Gil, Enrique García-Berro Montilla Data: 27 de juliol de 2009 Resum Gaia és una missió astromètrica de l'Agència Espacial Europea (ESA) amb l'ambiciós objectiu de fer el mapa en tres dimensions de la nostra Galàxia més gran i precís fet fins ara. Per aconseguir-ho Gaia escanejarà l'espai contínuament i proporcionarà informació molt precisa sobre la posició, velocitat i espectre d'aproximadament mil milions d'estrelles de la Via Làctia. Això proporcionarà una informació molt valuosa sobre la composició, formació i evolució de la nostra Galàxia. Gaia també detectarà milers de petits objectes del sistema solar, planetes extra-solars, galàxies llunyanes, etc. Per tal de fer les observacions el més precises possibles Gaia descriurà una òrbita de tipus Lissajous al voltant del punt Lagrangià L2 del sistema Sol-Terra. Aquesta és una òrbita molt adequada ja es molt estable. Així mateix, aquesta òrbita té una gran estabilitat tèrmica. A més té unes característiques d'observació molt bones ja que el Sol, la Terra, la Lluna i els planetes interiors estan sempre per darrere del camp d'observació. En aquest treball final de carrera, en un primer lloc, estudiarem les òrbites de Lissajous, simularem l'orbita de Lissajous prevista per la missió Gaia i analitzarem les seves característiques.