AIDA: Asteroid Impact & Deflection Assessment A Joint ESA-NASA Mission. Joint ESA NASA AIDA Team
|
|
- Dylan Crawford
- 8 years ago
- Views:
Transcription
1 AIDA: Asteroid Impact & Deflection Assessment A Joint ESA-NASA Mission Joint ESA NASA AIDA Team Chelyabinsk Meteor on 15 February 2013
2 AIDA Asteroid Deflection Test AIDA international cooperation First test of asteroid deflection by kinetic impact DART kinetic impactor (NASA) AIM rendezvous and impact monitoring (ESA) AIM Radar Telescopes DART Didymos Binary 1
3 AIDA = AIM + DART ESA AIM rendezvous spacecraft Orbiter payload to characterize Didymos dynamical system and study impact results characterisation Asteroid proximity operations, lander release on secondary asteroid, deep-interior analysis Deep-space optical communication demonstration NASA DART interceptor and Earth-based observing Measure asteroid deflection to within 10% Return high resolution images of target prior to impact Autonomous guidance with proportional navigation to hit center of 150 meter target body Leverage space-based missile technology 2
4 AIDA Relevance Science Conduct a visit to a binary near-earth asteroid Detect possible mass transfer between primary & secondary bodies Measure crater formation and redistribution of material Estimate internal structure and composition Planetary Defense Understand kinetic impact effects for future deflection technologies Estimate momentum transfer by impact and by enhancement of ejecta Exploration Coordinate international deep space mission operations Develop flight techniques and experience for small body missions Optical navigation and acquisition Rendezvous Proximity Operations Plan and perform detailed characterization Resources investigation 3
5 2022 Didymos Intercept DART trajectory remains near 1 AU from Sun, Earth distance < 0.11 AU. DART launch energy 3.74 km 2 /s 2 Impact velocity 6.27 km/s Impact event in Oct, 2022 occurs under excellent Earth-based viewing conditions including radar Co-manifest launch under study DART launches Dec 20, 2021 and intercepts Didymos on Oct 1,
6 AIDA Target Properties The target is the Near-Earth Asteroid (1996 GT) Didymos: a YORP spin-up binary with an equatorial ridge on the primary Binary 1999 KW4 radar model Ostro et al EV5 Busch et al Bennu NASA/NSF/Cornell/Nolan Radar image of Didymos From L. Benner, Arecibo, Nov
7 DART Payload Objectives DART payload is an imager based on New Horizons LORRI 20 cm telescope, 1 arc sec/px, CCD camera Support autonomous guiding to impact target body through center Determine impact point within 1% of target diameter Characterize pre-impact surface morphology and geology of target (goal <20 cm/px) and companion body 5/29/2012 6
8 AIM mission objectives Primary objectives 1 Determine the binary asteroid orbital and rotation dynamics, as well as the mass, geolophysical properties, and surface and subsurface structure; 2 to carry out a Telecommunication Engineering experiment (TEX), a Moonlet Engineering experiment (MEX) deploying the MASCOT-2 asteroid lander; 3 to test inter-satellite network link with COPINS (Cubesat Opportunity Payload Intersatellite Network Sensors) and the MASCOT-2 lander. Secondary objectives 4 to determine the momentum transfer resulting from the impact of the DART, by measuring the variation of the asteroid s period, its rotation state and by imaging of the resulting impact crater. An optional extension of this primary objective is the imaging the asteroid ejecta resulting from the impact. 5 to characterise the asteroid deep interior structure.
9 AIM main elements Technology Payload Mass OPTEL-D (Optical terminal) 39.3 MASCOT-2 (incl. low-frequency radar) 13 COPINS 13.2 Asteroid Research Payload Mass Thermal Infrared Imager 3.6 Monostatic High Frequency Radar 1.7 Bistatic Low Frequency Radar (Orbiter) 1.2 Visual Imaging Camera 2.4
10 AIM mission scenario DSM: 03/01/2021 Launch by Soyuz from Kourou: ~22/10/ Arrival 29/5/2022 ~35 km 6 2 ~100 km DART impact 6/10/ Launch 4 Rendezvous burn 7 DART impact observation 2 Departure burn 5 Co-flying / Characterisation 8 Co-flying / Characterisation 3 Deep space manoeuvre 6 Lander deployment 9 Post-impact characterisation
11 Close proximity Asteroid Operations: 29 May December 2022 P1 Rendezvous with Didymos Transition to 35 km P2 co-flying position. 35 km P2 Early characterization: - High-resolution images - Optical comm experiment ~1 km 10 km P3 First detailed characterization: Thermal Infrared imaging High-frequency radar sounding of surface and shallow-subsurface ~100 km P5 DART impact observation P4 Lander phase: Deploy MASCOT2 lander 10 km P6 Second detailed characterization: - High-frequency radar - Low-frequency radar - Crater imaging
12 CubeSats Opportunity Payloads (COPINS) Intersatellite link demonstration in deep space ESA AIM mothercraft AO in 1 st quarter 2015
13 AIM schedule Pre-phase A (ESA CDF) May - Sept 14 AIM AO Oct 14 Jan Phase-A (9 months) KO End of February 15 Preliminary requirements review Dec 15 Phase-B1 (6 months) Intermediate system requirements review June 16
14 DART Baseline Schedule May 2015 Feb 2016 Apr 2016 Jul 2016 Feb 2017 Jan 2018 Sep 2018 Apr 2019 Aug 2019 Jan 2020 MCR SRR/CoDR Instrument Phase B starts Bus/ground Phase B starts PDR CDR SIR PER PSR/ORR Launch 13
15 AIDA Since we last met. DART Pre-phase A study efforts continue Focus on modeling and simulation, algorithm development, AutoNav development, and primary sensor detector trades Continue to mature the integrated mission design: multiple launch opportunities available to support an October 2022 intercept of the Didymos binary system AIM Advisory Group report on Environmental and Instrumentation Requirements, issued April, 2014 Participated in the ESA AIM mission engineering (CDF) study (past summer) at ESTEC Multiple community interactions both in the US and Europe, including the.. 1 st International Community Workshop was held at APL October Formalizing the NASA-ESA partnership Telecon, and official NASA visit (November 17, 18) of Franco Ongaro, Head of ESA/ESTEC and Director of Technology Formalizing Letter of Intent to pursue Phase A/B1 in parallel 14
16 AIDA Next 6 months. DART will complete Pre-phase A study and transition to Phase A late Spring/early summer Next iteration design run in mid-march Co-manifest launch study continues MCR tentatively scheduled for late May 2015 Exploring teaming with other NASA directorates (stakeholders) Expand on community involvement and how to leverage other relevant efforts funded by both US and European NEO Programs Align joint milestone dates between DART and AIM (best effort) Our next AIDA international community forum will be during the Planetary Defense Conference in April 2015 ESA will down-select up to 3 industry system studies in late January 2015 European payload studies and early development will start in early 2015 ESA COPINS AO to be released Jan 2015 Joint US payload contributions to an ESA surface package will be studied 15
17 16
18 DART Impact Results Parameter β defined as orbital momentum change divided by momentum input Perfectly inelastic collision: β = 1 Ejecta enhances momentum transfer, β > 1 Assuming β = 1, the v is ~0.3 mm/s for Didymos satellite after DART impact; period change of ~200 s (out of ~12 hours) Period change detectable from Earth Imparted Δv, mm/s Δ semi-major axis, m Δ period, sec Δ period, % 0.48% 0.64% 0.80% 2.43% Δ eccentricity Δ inclination, deg Δ longitude of pericenter, ῶ = Ω+ω, deg
Robotic Pre-Cursor Contribution to Human NEA Mission. H. Kuninaka JSPEC/JAXA
Robotic Pre-Cursor Contribution to Human NEA Mission H. Kuninaka JSPEC/JAXA Asteroid Explorer Hayabusa Dimensions 1.0m x 1.6m x 1.1m Weight : 380kg(Dry) Chemical Fuel 70kg Xe Propellant 60kg Total 510kg
More informationESA studies on the Don Quijote NEO mission: dealing with impact uncertainties
IAC-05-Q.P.21 ESA studies on the Don Quijote NEO mission: dealing with impact uncertainties Andrés Gálvez 1, Ian Carnelli 2 1 Advanced Concepts and Studies Office, ESA HQ, 8-10 rue Mario Nikis 75738 Paris
More informationA STUDY OF THE ORBITAL DYNAMICS OF THE ASTEROID 2001 SN263.
O.C.Winter,2, R.A.N.Araujo, A.F.B.A.Prado, A.Sukhanov INPE- National Institute for Space Research, São José dos Campos,Brazil. 2 Sao Paulo State University, Guaratinguetá, Brazil. Abstract: The asteroid
More informationChapter 9 Asteroids, Comets, and Dwarf Planets. Their Nature, Orbits, and Impacts
Chapter 9 Asteroids, Comets, and Dwarf Planets Their Nature, Orbits, and Impacts Asteroid Facts Asteroids are rocky leftovers of planet formation. The largest is Ceres, diameter ~1,000 km. There are 150,000
More informationAT&T Global Network Client for Windows Product Support Matrix January 29, 2015
AT&T Global Network Client for Windows Product Support Matrix January 29, 2015 Product Support Matrix Following is the Product Support Matrix for the AT&T Global Network Client. See the AT&T Global Network
More informationInteraction of Energy and Matter Gravity Measurement: Using Doppler Shifts to Measure Mass Concentration TEACHER GUIDE
Interaction of Energy and Matter Gravity Measurement: Using Doppler Shifts to Measure Mass Concentration TEACHER GUIDE EMR and the Dawn Mission Electromagnetic radiation (EMR) will play a major role in
More informationPlanetary Defense! Space System Design, MAE 342, Princeton University! Robert Stengel
Planetary Defense! Space System Design, MAE 342, Princeton University! Robert Stengel!! Asteroids and Comets!! Spacecraft!! Detection, Impact Prediction, and Warning!! Options for Minimizing the Hazard!!
More informationORBITAL DISPERSION SIMULATION OF NEAR-EARTH OBJECT DEFLECTION/FRAGMENTATION BY NUCLEAR EXPLOSIONS
IAC-09-C1.10.2 ORBITAL DISPERSION SIMULATION OF NEAR-EARTH OBJECT DEFLECTION/FRAGMENTATION BY NUCLEAR EXPLOSIONS B. Kaplinger Iowa State University, United States bdkaplin@iastate.edu B. Wie Iowa State
More informationTask 329. Tracking and Monitoring Suborbital Commercial Space Vehicles
Task 329. Tracking and Monitoring Suborbital Commercial Space Vehicles Dr. William H. Ryan Research Faculty, 2.4-meter Telescope (NM Tech/Magdalena Ridge Observatory) Project Overview Ultimately: develop
More informationRS platforms. Fabio Dell Acqua - Gruppo di Telerilevamento
RS platforms Platform vs. instrument Sensor Platform Instrument The remote sensor can be ideally represented as an instrument carried by a platform Platforms Remote Sensing: Ground-based air-borne space-borne
More informationHyperspectral Satellite Imaging Planning a Mission
Hyperspectral Satellite Imaging Planning a Mission Victor Gardner University of Maryland 2007 AIAA Region 1 Mid-Atlantic Student Conference National Institute of Aerospace, Langley, VA Outline Objective
More informationCarry of Asteroids - A Guide to Asteroid Spreading
1/17 B. Carry, ERICE, 2015/10/13 Solar system science in the E-ELT era B. Carry 1,2 1 IMCCE, Observatoire de Paris 2 Lagrange, Observatoire de la Côte d Azur 2/17 B. Carry, ERICE, 2015/10/13 1. Contamination
More informationMars Sample Return Campaign: An Overview. Dr. Firouz Naderi Associate Director NASA s JPL
Mars Sample Return Campaign: An Overview Dr. Firouz Naderi Associate Director NASA s JPL 1 Why Sample Return? Why Now? Compelling Science Informed Landing Site Selection International Interest Good Engineering
More informationMission Spacecraft and Operations Overview MAVEN Science Community Workshop December 2, 2012
Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission Mission Spacecraft and Operations Overview MAVEN Science Community Workshop December 2, 2012 Chris Waters Spacecraft Design Lead Lockheed Martin MAVEN
More informationCOMPARISON OF FIXED & VARIABLE RATES (25 YEARS) CHARTERED BANK ADMINISTERED INTEREST RATES - PRIME BUSINESS*
COMPARISON OF FIXED & VARIABLE RATES (25 YEARS) 2 Fixed Rates Variable Rates FIXED RATES OF THE PAST 25 YEARS AVERAGE RESIDENTIAL MORTGAGE LENDING RATE - 5 YEAR* (Per cent) Year Jan Feb Mar Apr May Jun
More informationCOMPARISON OF FIXED & VARIABLE RATES (25 YEARS) CHARTERED BANK ADMINISTERED INTEREST RATES - PRIME BUSINESS*
COMPARISON OF FIXED & VARIABLE RATES (25 YEARS) 2 Fixed Rates Variable Rates FIXED RATES OF THE PAST 25 YEARS AVERAGE RESIDENTIAL MORTGAGE LENDING RATE - 5 YEAR* (Per cent) Year Jan Feb Mar Apr May Jun
More informationCongresso della SAIT Museo della Scienza e della Tecnologia di Milano 15 Maggio 2014
Congresso della SAIT Museo della Scienza e della Tecnologia di Milano 15 Maggio 2014 Francesca Esposito INAF Osservatorio Astronomico di Capodimonte (Napoli) ExoMars Mission The ExoMars Program is carried
More informationTrajectory design for the Solar Orbiter mission
Monografías de la Real Academia de Ciencias de Zaragoza. 25: 177 218, (2004). Trajectory design for the Solar Orbiter mission G. Janin European Space Operations Centre. European Space Agency. 64293 Darmstadt,
More informationDr. David Burns Director for Science and Technology Advanced Technology Missile Defense Agency
Dr. David Burns Director for Science and Technology Missile Defense Agency DISTRIBUTION STATEMENT A. ; Distribution is UNLIMITED. 13-MDA-7174 Modeling and Today s Ballistic Missile Defense System 13-MDA-7174
More informationSolar System Observations contains two components: Planetary Astronomy and Near Earth Object Observations.
C.6 SOLAR SYSTEM OBSERVATIONS 1. Scope of Program Solar System Observations supports both ground-based astronomical observations and suborbital investigations of our Solar System involving sounding rockets
More informationDawn - Overview, Science Objectives, Mission Progress. Hap McSween For PI Chris Russell
Dawn - Overview, Science Objectives, Mission Progress Hap McSween For PI Chris Russell Presentation to Decadal Survey Primitive Bodies Panel, Washington, DC, Sep 2009 Spacecraft configuration, assembly
More informationCBERS Program Update Jacie 2011. Frederico dos Santos Liporace AMS Kepler liporace@amskepler.com
CBERS Program Update Jacie 2011 Frederico dos Santos Liporace AMS Kepler liporace@amskepler.com Overview CBERS 3 and 4 characteristics Differences from previous CBERS satellites (CBERS 1/2/2B) Geometric
More informationDouglas Adams The Hitchhikers Guide to the Galaxy
There is a theory which states that if ever anybody discovers exactly what the Universe is for and why it is here, it will instantly disappear and be replaced by something even more bizarre and inexplicable.
More informationNASA Technology Roadmap Update Overview
National Aeronautics and Space Administration NASA Technology Roadmap Update Overview NASA Advisory Committee Technology, Innovation, and Engineering Committee Meeting December 4, 2014 Faith Chandler NASA
More informationPenn State University Physics 211 ORBITAL MECHANICS 1
ORBITAL MECHANICS 1 PURPOSE The purpose of this laboratory project is to calculate, verify and then simulate various satellite orbit scenarios for an artificial satellite orbiting the earth. First, there
More informationChang e-3 s Progress and Achievement 2/2014
Chang e-3 s Progress and Achievement 2/2014 Main content 1. Chinese Lunar Exploration Program 2. Chang e-3 s Progress 3. Chang e-3 s Achievement Chinese Lunar Exploration Program Phase I Orbital missions
More informationSolar Sailing Mission Opportunities and Innovative Technology Demonstration
r bulletin 108 november 2001 Solar Sailing Mission Opportunities and Innovative Technology Demonstration C.R. McInnes Department of Aerospace Engineering, University of Glasgow, Glasgow, United Kingdom
More informationCase 2:08-cv-02463-ABC-E Document 1-4 Filed 04/15/2008 Page 1 of 138. Exhibit 8
Case 2:08-cv-02463-ABC-E Document 1-4 Filed 04/15/2008 Page 1 of 138 Exhibit 8 Case 2:08-cv-02463-ABC-E Document 1-4 Filed 04/15/2008 Page 2 of 138 Domain Name: CELLULARVERISON.COM Updated Date: 12-dec-2007
More informationSSA NEO Segment. Overview and approach for Phase 2. Detlef Koschny, Gerhard Drolshagen Detlef.Koschny@esa.int
SSA NEO Segment Overview and approach for Phase 2 Detlef Koschny, Gerhard Drolshagen Detlef.Koschny@esa.int SSA NEO ESA HO 0140/1.0, Industry Day ESOC Image credit: ESA 1 Publ ESA Unclassified Releasable
More informationCrater detection with segmentation-based image processing algorithm
Template reference : 100181708K-EN Crater detection with segmentation-based image processing algorithm M. Spigai, S. Clerc (Thales Alenia Space-France) V. Simard-Bilodeau (U. Sherbrooke and NGC Aerospace,
More informationSection 4: The Basics of Satellite Orbits
Section 4: The Basics of Satellite Orbits MOTION IN SPACE VS. MOTION IN THE ATMOSPHERE The motion of objects in the atmosphere differs in three important ways from the motion of objects in space. First,
More informationRoles: Scrum Master & Project Manager
Roles: Scrum Master & Project Manager Scrum Master: Facilitate collaborative meetings Track team performance Remove impediments (Risk, Issue) Validate team alignment to Agile framework and scope Drive
More informationAGI Software for Space Situational Awareness
AGI Software for Space Situational Awareness The number of objects in space has significantly proliferated since 1957, with more than 17,000 objects bigger than 10 cm and 1,000+ active payloads currently
More informationThe Threat of Orbital Debris and Protecting NASA Space Assets from Satellite Collisions 28 April 2009
The Threat of Orbital Debris and Protecting NASA Space Assets from Satellite Collisions 28 April 2009 Executive Summary Collision avoidance processes are in place for all NASA human space flight missions
More informationTelepresence for Deep Space Missions Project
ABSTRACT Incorporating telepresence technologies into deep space mission operations can give the crew and ground personnel the impression that they are in a location at time that they are not. NASA s space
More informationSolar Sails for Space Exploration The Development and Demonstration of Critical Technologies in Partnership
r bulletin 98 june 1999 Solar Sails for Space Exploration The Development and Demonstration of Critical Technologies in Partnership M. Leipold Institute of Space Sensor Technology and Planetary Exploration,
More informationAPOPHIS 2029 A UNIQUE MISSION OPPORTUNITY
APOPHIS 2029 A UNIQUE MISSION OPPORTUNITY Jean-Yves Prado CNES Toulouse - France Presentation Outline APOPHIS reminder The April 2029 flyby Mission objectives Sequence of events Launch Orbit transfer Relative
More informationStatistical Vertical Turbulence Profiles at the Canary Islands Astronomical Sites
Statistical Vertical Turbulence Profiles at the Canary Islands Astronomical Sites B. García-Lorenzo 1, J.J. Fuensalida 1, J. Castro-Almazán 1, & M.A.C. Rodríguez-Hernández 1 (1) Instituto de Astrofísica
More informationLecture L17 - Orbit Transfers and Interplanetary Trajectories
S. Widnall, J. Peraire 16.07 Dynamics Fall 008 Version.0 Lecture L17 - Orbit Transfers and Interplanetary Trajectories In this lecture, we will consider how to transfer from one orbit, to another or to
More informationEN4 Dynamics and Vibrations. Design Project. Orbital Design for a Lunar Impact Mission. Synopsis
EN4 Dynamics and Vibrations Design Project Orbital Design for a Lunar Impact Mission Synopsis NASA has identified a need for a low-cost mission to launch a satellite that will impact the moon. You will
More informationNASA s Dawn Mission Journey to the Asteroid Frontier
NASA s Dawn Mission Journey to the Asteroid Frontier Dawn Lucy McFadden, Co-Investigator University of Maryland College Park, MD January 12, 2009 SBAG update 9 th Discovery Mission Dawn Explores the Earliest
More informationEnhanced Vessel Traffic Management System Booking Slots Available and Vessels Booked per Day From 12-JAN-2016 To 30-JUN-2017
From -JAN- To -JUN- -JAN- VIRP Page Period Period Period -JAN- 8 -JAN- 8 9 -JAN- 8 8 -JAN- -JAN- -JAN- 8-JAN- 9-JAN- -JAN- -JAN- -JAN- -JAN- -JAN- -JAN- -JAN- -JAN- 8-JAN- 9-JAN- -JAN- -JAN- -FEB- : days
More informationBinary and Multiple Systems
Binary and Multiple Systems Andrew Cheng 1, Andrew Rivkin 2, Patrick Michel 3, Carey Lisse 4, Kevin Walsh 5, Keith Noll 6, Darin Ragozzine 7, Clark Chapman 8, William Merline 9, Lance Benner 10, Daniel
More informationAstromechanics Two-Body Problem (Cont)
5. Orbit Characteristics Astromechanics Two-Body Problem (Cont) We have shown that the in the two-body problem, the orbit of the satellite about the primary (or vice-versa) is a conic section, with the
More informationAutomated Spacecraft Scheduling The ASTER Example
Automated Spacecraft Scheduling The ASTER Example Ron Cohen ronald.h.cohen@jpl.nasa.gov Ground System Architectures Workshop 2002 Jet Propulsion Laboratory The Concept Scheduling by software instead of
More informationBUILDING TRANSATLANTIC PARTNERSHIPS IN SPACE EXPLORATION THE MPCV-SM STUDY
BUILDING TRANSATLANTIC PARTNERSHIPS IN SPACE EXPLORATION THE MPCV-SM STUDY Following the approval of the ESA ISS Exploitation Declaration for the ISS lifetime at the ESA Council Meeting in March 2011,
More informationAsteroid Deflection Theory: fundamentals of orbital mechanics and optimal control
Asteroid Deflection Theory: fundamentals of orbital mechanics and optimal control D. Izzo, J. Olympio, C. H. Yam (1) (1) ESA, Advanced Concepts Team, ESTEC, Keplerlaan 1, Postbus 299, 2200 AG, Noordwijk
More informationA remote sensing instrument collects information about an object or phenomenon within the
Satellite Remote Sensing GE 4150- Natural Hazards Some slides taken from Ann Maclean: Introduction to Digital Image Processing Remote Sensing the art, science, and technology of obtaining reliable information
More informationCommercial Crew Program Status
National Aeronautics and Space Administration Commercial Crew Program Status for the NAC Presenter Title Date Philip McAlister of Presentation Acting Director, Commercial Spaceflight Development NASA HQ
More informationOrbital Mechanics. Angular Momentum
Orbital Mechanics The objects that orbit earth have only a few forces acting on them, the largest being the gravitational pull from the earth. The trajectories that satellites or rockets follow are largely
More informationScience and Technology Challenges in Near-Earth Space Weather Dr. Larry J. Paxton Space Department The Johns Hopkins University Applied Physics Laboratory Overview and Challenges Space weather, particularly
More informationTropical Horticulture: Lecture 2
Lecture 2 Theory of the Tropics Earth & Solar Geometry, Celestial Mechanics The geometrical relationship between the earth and sun is responsible for the earth s climates. The two principal movements of
More informationPhysics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam
Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam INSTRUCTIONS: Use a pencil #2 to fill your scantron. Write your code number and bubble it in under "EXAM NUMBER;" an entry
More informationForest Fire Information System (EFFIS): Rapid Damage Assessment
Forest Fire Information System (EFFIS): Fire Danger D Rating Rapid Damage Assessment G. Amatulli, A. Camia, P. Barbosa, J. San-Miguel-Ayanz OUTLINE 1. Introduction: what is the JRC 2. What is EFFIS 3.
More informationHalliday, Resnick & Walker Chapter 13. Gravitation. Physics 1A PHYS1121 Professor Michael Burton
Halliday, Resnick & Walker Chapter 13 Gravitation Physics 1A PHYS1121 Professor Michael Burton II_A2: Planetary Orbits in the Solar System + Galaxy Interactions (You Tube) 21 seconds 13-1 Newton's Law
More informationHayabusa2. Presented by Paul Abell. H. Kuninaka, N. Inaba, Y. Tsuda, M. Yoshikawa (JAXA) SBAG, Washington DC, USA 29 July 2014 HAYABUSA2 1999JU3
Hayabusa2 HAYABUSA2 1999JU3 SBAG, Washington DC, USA 29 July 2014 Presented by Paul Abell H. Kuninaka, N. Inaba, Y. Tsuda, M. Yoshikawa (JAXA) Current Status We are now doing final integration test, which
More informationASTEROID IMPACT MISSION: DIDYMOS REFERENCE MODEL
headquarters 8-1o rue Mario Nikis 75738 Cedex 15 Paris France www.esa.int ASTEROID IMPACT MISSION: DIDYMOS REFERENCE MODEL Issue 1 Revision Date of Issue 5 05/03/15 Status Released Document Type AD Table
More informationF N A) 330 N 0.31 B) 310 N 0.33 C) 250 N 0.27 D) 290 N 0.30 E) 370 N 0.26
Physics 23 Exam 2 Spring 2010 Dr. Alward Page 1 1. A 250-N force is directed horizontally as shown to push a 29-kg box up an inclined plane at a constant speed. Determine the magnitude of the normal force,
More informationAstrodynamics (AERO0024)
Astrodynamics (AERO0024) 6. Interplanetary Trajectories Gaëtan Kerschen Space Structures & Systems Lab (S3L) Course Outline THEMATIC UNIT 1: ORBITAL DYNAMICS Lecture 02: The Two-Body Problem Lecture 03:
More informationAnalysis One Code Desc. Transaction Amount. Fiscal Period
Analysis One Code Desc Transaction Amount Fiscal Period 57.63 Oct-12 12.13 Oct-12-38.90 Oct-12-773.00 Oct-12-800.00 Oct-12-187.00 Oct-12-82.00 Oct-12-82.00 Oct-12-110.00 Oct-12-1115.25 Oct-12-71.00 Oct-12-41.00
More informationSmall Satellite Space Traffic Management
Small Satellite Space Traffic Management Brian Weeden Technical Advisor Secure World Foundation 1 THE SHIFT FROM BIG SATELLITES TO SMALL ONES 2 Historically, satellites were large and complex machines
More informationPRELIMINARY DESIGN OF A HYPERVELOCITY NUCLEAR INTERCEPTOR SYSTEM (HNIS) FOR OPTIMAL DISRUPTION OF NEAR-EARTH OBJECTS
AAS 12-225 PRELIMINARY DESIGN OF A HYPERVELOCITY NUCLEAR INTERCEPTOR SYSTEM (HNIS) FOR OPTIMAL DISRUPTION OF NEAR-EARTH OBJECTS Alan Pitz, Brian Kaplinger, and Bong Wie and David Dearborn When the warning
More information7th Agile Meeting & The Bright Gamma-Ray Sky Frascati, 29 September - 1 October, 2009. Carlotta Pittori, on behalf of the ADC
7th Agile Meeting & The Bright Gamma-Ray Sky Frascati, 29 September - 1 October, 2009 The AGILE Data Center and the First AGILE Catalog Carlotta Pittori, on behalf of the ADC AGILE GS Architecture Fucino,
More informationSearching for space debris elements with the Pi of the Sky system
Searching for space debris elements with the Pi of the Sky system Marcin Sokołowski msok@fuw.edu.pl Soltan Institute for Nuclear Studies ( IPJ ) Warsaw, Poland 7th Integral / BART Workshop ( IBWS), 14-18
More informationLaguduva Kubendran, PhD, MBA Program Executive, NASA HQ GSFC Emerging Commercial Suborbital Capabilities Workshop September 7, 2011. www.nasa.
Laguduva Kubendran, PhD, MBA Program Executive, NASA HQ GSFC Emerging Commercial Suborbital Capabilities Workshop September 7, 2011 www.nasa.gov Office of the Chief Technologist Program Map Space Tech
More informationA science class experience that is out of this world. Robert Benkoczi, PhD Optimization Research Group University of Lethbridge
A science class experience that is out of this world Robert Benkoczi, PhD Optimization Research Group University of Lethbridge SWATCA 2015 Summary Optimization Research Group Funcube project and reception
More informationThis paper is also taken for the relevant Examination for the Associateship. For Second Year Physics Students Wednesday, 4th June 2008: 14:00 to 16:00
Imperial College London BSc/MSci EXAMINATION June 2008 This paper is also taken for the relevant Examination for the Associateship SUN, STARS, PLANETS For Second Year Physics Students Wednesday, 4th June
More informationProgress of MoonLITE Penetrators
Progress of MoonLITE Penetrators Rob Gowen on behalf of the UK Penetrator Consortium Brief overview Status Phase-A A elements Impact Trial Collaboration Contents MoonLITE Mission A UK led science mission
More informationThe European Satellite Navigation Programmes EGNOS and Galileo
The European Satellite Navigation Programmes EGNOS and Galileo Olivier Crop European GNSS Agency (GSA) Paris, 17 March 2014 20 March, 2014 The European GNSS Programmes 2 Basics of Satellite Navigation
More informationRobot Perception Continued
Robot Perception Continued 1 Visual Perception Visual Odometry Reconstruction Recognition CS 685 11 Range Sensing strategies Active range sensors Ultrasound Laser range sensor Slides adopted from Siegwart
More informationExamination Space Missions and Applications I (AE2103) Faculty of Aerospace Engineering Delft University of Technology SAMPLE EXAM
Examination Space Missions and Applications I AE2103 Faculty of Aerospace Engineering Delft University of Technology SAMPLE EXAM Please read these instructions first: This are a series of multiple-choice
More informationSolar Power for Outer Planets Study
Solar Power for Outer Planets Study Presentation to Outer Planets Assessment Group November 8, 2007 Scott W. Benson/NASA Glenn Research Center 1 Background & Outline Alan Stern request: a quick look study
More informationCan Hubble be Moved to the International Space Station? 1
Can Hubble be Moved to the International Space Station? 1 On January 16, NASA Administrator Sean O Keefe informed scientists and engineers at the Goddard Space Flight Center (GSFC) that plans to service
More informationTRACKING DATA MESSAGE. PROTOTYPING TEST PLAN Draft #1
TRACKING DATA MESSAGE PROTOTYPING TEST PLAN Draft #1 16-Apr-2007 Table of Contents 1. Introduction...3 2. Blue Book Promotion Criteria... 3 3. Tracking Data Message (TDM) Testing Goals... 3 4. Test Overview...
More informationDEOS. Deutsche Orbitale Servicing Mission. The In-flight Technology Demonstration of Germany s Robotics Approach to Service Satellites
DEOS Deutsche Orbitale Servicing Mission The In-flight Technology Demonstration of Germany s Robotics Approach to Service Satellites B. Sommer, K. Landzettel, T. Wolf, D. Reintsema, German Aerospace Center
More informationSpace Flight Project Work Breakdown Structure
APPENDIX G. (WBS) Space Flight Project Work Breakdown Structure G.1 Introduction G.1.1 The Project Work Breakdown Structure (WBS) is a key element of project management. The purpose of a WBS is to divide
More informationScience 9 Worksheet 13-1 The Solar System
Name Date Due Date Science 9 Read pages 264-287 of SP to help you answer the following questions: Also, go to a school computer connected to the internet. Go to Mr. Colgur s Webpage at http://sd67.bc.ca/teachers/dcolgur
More informationTHE MASTER PLAN CAMPAIGN. Workshop RPAS (WS 03) 22 January 2015
THE MASTER PLAN CAMPAIGN Workshop RPAS (WS 03) 22 January 2015 Back-up The objectives of the campaign 2 Campaign objectives Following the endorsement from the PC, SPP and ADB of the PC Tiger Team recommendations
More informationChapter 12 Asteroids, Comets, and Dwarf Planets. Asteroid Facts. What are asteroids like? Asteroids with Moons. 12.1 Asteroids and Meteorites
Chapter 12 Asteroids, Comets, and Dwarf Planets Their Nature, Orbits, and Impacts What are asteroids like? 12.1 Asteroids and Meteorites Our goals for learning:! What are asteroids like?! Why is there
More informationHalliday, Resnick & Walker Chapter 13. Gravitation. Physics 1A PHYS1121 Professor Michael Burton
Halliday, Resnick & Walker Chapter 13 Gravitation Physics 1A PHYS1121 Professor Michael Burton II_A2: Planetary Orbits in the Solar System + Galaxy Interactions (You Tube) 21 seconds 13-1 Newton's Law
More informationStatement of Dr. James Green Director, Planetary Science Division, Science Mission Directorate National Aeronautics and Space Administration
Statement of Dr. James Green Director, Planetary Science Division, Science Mission Directorate National Aeronautics and Space Administration before the Subcommittee on Space Committee on Science, Space
More informationDSL Mission Concept at Lunar Orbit
DSL Mission Concept at Lunar Orbit Jingye Yan Na9onal Space Science Center (NSSC) Chinese Academy of Sciences (CAS) 2015-02- 02, ASTRON, The Netherland 1 Payload onboard single nano- sat Element antenna
More informationPlanetary Orbit Simulator Student Guide
Name: Planetary Orbit Simulator Student Guide Background Material Answer the following questions after reviewing the Kepler's Laws and Planetary Motion and Newton and Planetary Motion background pages.
More informationWide Area Persistent Scatterer Interferometry: Algorithms and Examples
Wide Area Persistent Scatterer Interferometry: Algorithms and Examples Nico Adam, Fernando Rodriguez Gonzalez, Alessandro Parizzi, Werner Liebhart with contributions of Ramon Brcic and Xiao Ying Cong ca.
More informationScience Standard 4 Earth in Space Grade Level Expectations
Science Standard 4 Earth in Space Grade Level Expectations Science Standard 4 Earth in Space Our Solar System is a collection of gravitationally interacting bodies that include Earth and the Moon. Universal
More informationSpace Launch System Status Briefing to NAC Space Operations Committee
National Aeronautics and Space Administration Space Launch System Status Briefing to NAC Space Operations Committee 8 February 2011 Background In response to direction in Section 309 of the NASA Authorization
More informationCENTERPOINT ENERGY TEXARKANA SERVICE AREA GAS SUPPLY RATE (GSR) JULY 2015. Small Commercial Service (SCS-1) GSR
JULY 2015 Area (RS-1) GSR GSR (LCS-1) Texarkana Incorporated July-15 $0.50690/Ccf $0.45450/Ccf $0.00000/Ccf $2.85090/MMBtu $17.52070/MMBtu Texarkana Unincorporated July-15 $0.56370/Ccf $0.26110/Ccf $1.66900/Ccf
More informationThe USGS Landsat Big Data Challenge
The USGS Landsat Big Data Challenge Brian Sauer Engineering and Development USGS EROS bsauer@usgs.gov U.S. Department of the Interior U.S. Geological Survey USGS EROS and Landsat 2 Data Utility and Exploitation
More informationIodine RF Ion Thruster Development Busek Co. Inc. Vlad Hruby PhD, President
Iodine RF Ion Thruster Development Busek Co. Inc. Vlad Hruby PhD, President Mike Tsay PhD busek.com 2015 Busek Co. Inc. All Rights Reserved. Iodine RF Ion Thruster Development Status Briefing NASA NRA
More informationEXOMARS 2018 LANDING SITE PROPOSAL GUIDE & TEMPLATE
EXOMARS 2018 LANDING SITE PROPOSAL GUIDE & TEMPLATE Introduction: Ref: EXM-SCI-LSS-ESA/IKI-002 Version 1.0, 17 December 2013 Proposals are required to contain the following sections: 1) An abstract summarising
More informationSputnik and the Space Race. By: AJ Scangamor and Joseph Reed
Sputnik and the Space Race By: AJ Scangamor and Joseph Reed Background After WWII ended the Cold War had just begun. Within this war between two great powers competed in the battle of the Space Race, the
More informationUse the following information to deduce that the gravitational field strength at the surface of the Earth is approximately 10 N kg 1.
IB PHYSICS: Gravitational Forces Review 1. This question is about gravitation and ocean tides. (b) State Newton s law of universal gravitation. Use the following information to deduce that the gravitational
More informationSIMULATING SATELLITE DOWNLINK DATA LOSS AND RECOVERY DUE TO RAIN ATTENUATION
Proceedings of the 213 Winter Simulation Conference R. Pasupathy, S.-H. Kim, A. Tolk, R. Hill, and M. E. Kuhl, eds SIMULATING SATELLITE DOWNLINK DATA LOSS AND RECOVERY DUE TO RAIN ATTENUATION Douglas Shannon
More informationMain Belt Comets. Asteroid belt s new class of objects and possible source of water and volatiles for the Earth
Main Belt Comets Asteroid belt s new class of objects and possible source of water and volatiles for the Earth A science white paper submitted to Astro2010 Decadal Survey (Planetary Systems and Star Formation)
More informationThe Moon. Nicola Loaring, SAAO
The Moon Nicola Loaring, SAAO Vital Statistics Mean distance from Earth Orbital Period Rotational Period Diameter 384,400 km 27.322 days 27.322 days 3476 km (0.272 x Earth) Mass 7.3477 10 22 kg (0.0123
More informationNeutron Stars. How were neutron stars discovered? The first neutron star was discovered by 24-year-old graduate student Jocelyn Bell in 1967.
Neutron Stars How were neutron stars discovered? The first neutron star was discovered by 24-year-old graduate student Jocelyn Bell in 1967. Using a radio telescope she noticed regular pulses of radio
More informationFig.1. The DAWN spacecraft
Introduction Optical calibration of the DAWN framing cameras G. Abraham,G. Kovacs, B. Nagy Department of Mechatronics, Optics and Engineering Informatics Budapest University of Technology and Economics
More informationChange Management Advisory Council. September, 2010
Change Management Advisory Council September, 2010 Agenda 8:00-8:20: 8:20-8:40: 8:40-9:00: 9:00-9:30: Introduce team; share role of Advisory Council and discussion questions Discuss program overview and
More informationNASA Space Technology Programs ISS Research and Development Conference June 27, 2012 Richard B. Leshner, Ph.D. Program Executive SBIR/STTR
NASA Space Technology Programs ISS Research and Development Conference June 27, 2012 Richard B. Leshner, Ph.D. Program Executive SBIR/STTR Office of the Chief Technologist In 2010 NASA established the
More informationA Fractionated Space Weather Base at L 5 using CubeSats & Solar Sails
A Fractionated Space Weather Base at L 5 using CubeSats & Solar Sails Paulett C. Liewer, Andrew T. Klesh, Martin W. Lo, Neil Murphy, Robert L. Staehle, Vassilis Angelopoulos, Jet Propulsion Laboratory,
More information