Autonomous Formation Flying and Proximity Operations using Differential Drag on the Mars Atmosphere

Size: px
Start display at page:

Download "Autonomous Formation Flying and Proximity Operations using Differential Drag on the Mars Atmosphere"

Transcription

1 Autonomous Formation Flying and Proximity Operations using Differential Drag on the Mars Atmosphere Andrés E. Villa M.S. in Aerospace Engineering candidate California Polytechnic State University May 5 th, 2016

2 Agenda Introduction Mars facts Literature review Methods Results Pending work Conclusions 2

3 Introduction Motivation Why Mars? Why aerodynamic drag? Why formation flying? Why autonomous? 3

4 Introduction Feasibility Analysis A feasibility analysis was conducted showing that differential drag can be applied in Low Mars Orbits of 220 kilometers in altitude (maximum) Two different areas exposed to drag were simulated, obtaining enough drag to be used as means of control A paper was written and will be published 4

5 5 Acceleration due to atmospheric drag when the biggest area faces the Ram direction

6 6 Acceleration due to atmospheric drag when the smallest area faces the Ram direction

7 Introduction Purpose of the Study Use existing differential drag techniques Same as for Earth, but for Mars atmosphere Minimize the fuel used Cost reduction Finite resource Contamination / distortion 7

8 Introduction Research Questions Is it possible to use the same formulation as for Earth atmosphere? How different is the Martian atmosphere with respect to Earth? Is the Martian atmosphere enough dense to perform formation flying around it? How much time will be needed to constitute a formation? 8

9 Introduction Significance to the Field Mars aerobraking techniques already exist and have been proven to work, but No previous work has been done to demonstrate that formation flying is possible Means of control in finite time Requirements Limitations 9

10 Introduction Definitions Chief, Leader, Target Deputy, Follower, Chaser Ephemeris Time Data kernel Aberration due to communication delay 10

11 Introduction Limitations In-track maneuvers only No Solar Radiation Pressure was considered for Mars Each spacecraft has to know the navigation information of the other spacecraft involved GPS-like navigation system Inter-spacecraft communication system 11

12 Mars facts (compared to Earth) Parameter Earth Mars Mean radius 6378 kilometers kilometers Tilt of axis 23.5 degrees 25 degrees J2 harmonics (55% greater than on Earth) Solar irradiance 1378 kw/m kw/m 2 Length of day 23 hours 56 minutes 24 hours 37 minutes Length of year days 687 Earth days Atmosphere Nitrogen, Oxygen, Argon, others Mostly carbon dioxide, H20 vapor 12

13 Literature Review Extensive review conducted More than 15 papers are relevant to the field Differential drag Flight dynamics with linearized J2 perturbations Control techniques Autonomy requirements Only a couple are specific for Mars Multi-spacecraft navigation Mars atmosphere 13

14 Methods Introduction Two Mars atmospheric models available NASA s Mars-GRAM ESA s Mars Climate Database (MCD) Simulation using MATLAB Wrapper to access MCD FORTRAN routines for atmospheric models Wrapper to use Navigation and Ancillary Information Facility (NAIF) to store information 14

15 Methods Setting Two 6U CubeSat flying in a co-planar circular orbit at 220 kilometers Use of Schweighart-Sedwick equations Including linearized J2 perturbations Used to describe relative motion Optimal control being implemented Cost function such to minimize rendezvous time 15

16 Schweighart and Sedwick equations Satellite Motion Relative to a Second Satellite x = x 0 cos nt 1 s + 1 s s y 0 sin nt 1 s y = s 1 s x 0 sin nt 1 s + y 0 cos nt 1 s z = lt + m sin qt + φ s = 3J 2R e 2 8r ref cos 2i ref 16

17 Results As suggested in literature, integration time of 3 minutes can be used Preliminary results have been obtained to demonstrate feasibility of using same techniques on Mars atmosphere Analyzing theory of Lossless Convexification and Linear Programming methods 17

18 Pending work Finish implementing the optimal control Code fails to run. Now debugging. Finish writing the report Results of optimal control Comparison with Lossless Convexification Comparison with Linear Programming Writing conclusions Finish presentation for defense 18

19 Conclusions (as for now) Earth Formation flying techniques can be applied to Mars, where optimal control is desirable to minimize the time required to rendezvous Availability of Mars atmospheric models allows to implement high fidelity simulations Mars atmosphere is dense enough to perform formation flying missions 19

20 Questions?

AUTONOMOUS FORMATION FLYING AND PROXIMITY OPERATIONS USING DIFFERENTIAL DRAG ON THE MARS ATMOSPHERE

AUTONOMOUS FORMATION FLYING AND PROXIMITY OPERATIONS USING DIFFERENTIAL DRAG ON THE MARS ATMOSPHERE AUTONOMOUS FORMATION FLYING AND PROXIMITY OPERATIONS USING DIFFERENTIAL DRAG ON THE MARS ATMOSPHERE A Thesis presented to the Faculty of California Polytechnic State University, San Luis Obispo In Partial

More information

Feedback Control of Spacecraft Rendezvous Maneuvers using Differential Drag

Feedback Control of Spacecraft Rendezvous Maneuvers using Differential Drag Feedback Control of Spacecraft Rendezvous Maneuvers using Differential Drag D. Pérez 1 and R. Bevilacqua Rensselaer Polytechnic Institute, Troy, New York, 1180 This work presents a feedback control strategy

More information

Guidance and Control for Spacecraft Planar Re-phasing via Input Shaping and Differential Drag

Guidance and Control for Spacecraft Planar Re-phasing via Input Shaping and Differential Drag Università Sapienza, Dipartimento di Matematica March 5th, 014 Guidance and Control for Spacecraft Planar Re-phasing via Input Shaping and Differential Drag Riccardo Bevilacqua Rensselaer Polytechnic Institute

More information

Formation Flying and Rendezvous and Docking Simulator for Exploration Missions (FAMOS-V2)

Formation Flying and Rendezvous and Docking Simulator for Exploration Missions (FAMOS-V2) Formation Flying and Rendezvous and Docking Simulator for Exploration Missions (FAMOS-V2) Galder Bengoa, F. Alonso, D. García, M. Graziano (GMV S.A.) Dr. Guillermo Ortega (ESA/ESTEC) 2nd ESA Workshop on

More information

Lyapunov-based Spacecraft Rendezvous Maneuvers using Differential Drag

Lyapunov-based Spacecraft Rendezvous Maneuvers using Differential Drag AIAA Guidance, Navigation, and Control Conference 08-11 August 2011, Portland, Oregon AIAA 2011-6630 Lyapunov-based Spacecraft Rendezvous Maneuvers using Differential Drag D. Pérez 1 and R. Bevilacqua

More information

An Analysis of N-Body Trajectory Propagation. Senior Project. In Partial Fulfillment. of the Requirements for the Degree

An Analysis of N-Body Trajectory Propagation. Senior Project. In Partial Fulfillment. of the Requirements for the Degree An Analysis of N-Body Trajectory Propagation Senior Project In Partial Fulfillment of the Requirements for the Degree Bachelor of Science in Aerospace Engineering by Emerson Frees June, 2011 An Analysis

More information

Advanced Guidance Algorithms for Spacecraft Formation-keeping

Advanced Guidance Algorithms for Spacecraft Formation-keeping Advanced Guidance Algorithms for Spacecraft Formation-keeping Michael Tillerson and Jonathan P. How Space Systems Laboratory Massachusetts Institute of Technology Abstract This paper presents advanced

More information

SPACE DEBRIS CHASER CONSTELLATION

SPACE DEBRIS CHASER CONSTELLATION THE VISION SPACE DEBRIS CHASER CONSTELLATION Constellation management Application to SSO debris Inclination between 98 and 99.5 Altitude between 750 km and 850 km Constellation of 38 Cubesats Low-thrust

More information

FORMATION FLYING WITH SHEPHERD SATELLITES NIAC Fellows Meeting Michael LaPointe Ohio Aerospace Institute

FORMATION FLYING WITH SHEPHERD SATELLITES NIAC Fellows Meeting Michael LaPointe Ohio Aerospace Institute FORMATION FLYING WITH SHEPHERD SATELLITES 2001 NIAC Fellows Meeting Michael LaPointe Ohio Aerospace Institute WHAT IS FORMATION FLYING? Two or more satellites flying in prescribed orbits at a fixed separation

More information

Space Travel on a Shoestring: CubeSat Beyond LEO

Space Travel on a Shoestring: CubeSat Beyond LEO Space Travel on a Shoestring: CubeSat Beyond LEO Massimiliano Vasile, Willem van der Weg, Marilena Di Carlo Department of Mechanical and Aerospace Engineering University of Strathclyde, Glasgow 5th Interplanetary

More information

Pico-Satellite Orbit Control by Vacuum Arc Thrusters as Enabling Technology for Formations of Small Satellites

Pico-Satellite Orbit Control by Vacuum Arc Thrusters as Enabling Technology for Formations of Small Satellites 1/25 Pico-Satellite Orbit Control by Vacuum Arc Thrusters as Enabling Technology for Formations of Small Satellites Igal Kronhaus, Mathias Pietzka, Klaus Schilling, Jochen Schein Department of Computer

More information

Relative Orbital Elements: Theory and Applications

Relative Orbital Elements: Theory and Applications aa.stanford.edu stanford.edu Relative Orbital Elements: Theory and Applications Simone D Amico, PhD Assist. Prof. of Aeronautics and Astronautics Director, Space Rendezvous Laboratory (SLAB) Slide 1 Table

More information

ABSTRACT 1. INTRODUCTION

ABSTRACT 1. INTRODUCTION Force Modeling and State Propagation for Navigation and Maneuver Planning for CubeSat Rendezvous, Proximity Operations, and Docking Christopher W. T. Roscoe, Jacob D. Griesbach, Jason J. Westphal, Dean

More information

Constraint Based Control Method For Precision Formation Flight of Spacecraft AAS

Constraint Based Control Method For Precision Formation Flight of Spacecraft AAS Constraint Based Control Method For Precision Formation Flight of Spacecraft AAS 06-122 Try Lam Jet Propulsion Laboratory California Institute of Technology Aaron Schutte Aerospace Corporation Firdaus

More information

Distributed Coordination and Control of Formation Flying Spacecraft

Distributed Coordination and Control of Formation Flying Spacecraft Distributed Coordination and Control of Formation Flying Spacecraft Michael Tillerson, Louis Breger, and Jonathan P. How MIT Department of Aeronautics and Astronautics {mike t, lbreger, jhow}@mit.edu Abstract

More information

HERA MISSION & CM16 lessons learned

HERA MISSION & CM16 lessons learned HERA MISSION HERA MISSION & CM16 lessons learned (CM16) Schedule criticality for 2020 launch Prepare Asteroid mission with launch opportunities in 2023 (with back-up in 2024 and 2025) (CM16) Payload selection

More information

Using Differential Aerodynamic Forces for CubeSat Orbit Control Sanny R. Omar

Using Differential Aerodynamic Forces for CubeSat Orbit Control Sanny R. Omar A UBURN UNIVERSITY JOURNAL OF UNDERGRADUATE SCHOLARSHIP SPRING 2014 Using Differential Aerodynamic Forces for CubeSat Orbit Control Sanny R. Omar Abstract The focus of this paper is the use of aerodynamic

More information

Lunar Satellite Attitude Determination System

Lunar Satellite Attitude Determination System Lunar Satellite Attitude Determination System SENIOR DESIGN PROPOSAL PRESENTATION TEAM EPOCH KUPOLUYI, TOLULOPE (LEAD DEVELOPER) SONOIKI, OLUWAYEMISI (LEAD RESEARCHER) WARREN, DANAH (PROJECT MANAGER) NOVEMBER

More information

Figure 1. View of ALSAT-2A spacecraft

Figure 1. View of ALSAT-2A spacecraft ALSAT-2A TRANSFER AND FIRST YEAR OPERATIONS M. Kameche (1), A.H. Gicquel (2), D. Joalland (3) (1) CTS/ASAL, 1 Avenue de la Palestine, BP 13, Arzew 31200 Oran, Algérie, email:mo_kameche@netcourrier.com

More information

MULTI PURPOSE MISSION ANALYSIS DEVELOPMENT FRAMEWORK MUPUMA

MULTI PURPOSE MISSION ANALYSIS DEVELOPMENT FRAMEWORK MUPUMA MULTI PURPOSE MISSION ANALYSIS DEVELOPMENT FRAMEWORK MUPUMA Felipe Jiménez (1), Francisco Javier Atapuerca (2), José María de Juana (3) (1) GMV AD., Isaac Newton 11, 28760 Tres Cantos, Spain, e-mail: fjimenez@gmv.com

More information

MARS DROP. Matthew A. Eby Mechanical Systems Department. Vehicle Systems Division/ETG The Aerospace Corporation May 25, 2013

MARS DROP. Matthew A. Eby Mechanical Systems Department. Vehicle Systems Division/ETG The Aerospace Corporation May 25, 2013 MARS DROP Matthew A. Eby Mechanical Systems Department Vehicle Systems Division/ETG The Aerospace Corporation May 25, 2013 The Aerospace Corporation 2013 The Aerospace Corporation (Aerospace), a California

More information

Control of Long-Term Low-Thrust Small Satellites Orbiting Mars

Control of Long-Term Low-Thrust Small Satellites Orbiting Mars SSC18-PII-26 Control of Long-Term Low-Thrust Small Satellites Orbiting Mars Christopher Swanson University of Florida 3131 NW 58 th Blvd. Gainesville FL ccswanson@ufl.edu Faculty Advisor: Riccardo Bevilacqua

More information

ORBITAL DECAY PREDICTION AND SPACE DEBRIS IMPACT ON NANO-SATELLITES

ORBITAL DECAY PREDICTION AND SPACE DEBRIS IMPACT ON NANO-SATELLITES Journal of Science and Arts Year 16, No. 1(34), pp. 67-76, 2016 ORIGINAL PAPER ORBITAL DECAY PREDICTION AND SPACE DEBRIS IMPACT ON NANO-SATELLITES MOHAMMED CHESSAB MAHDI 1 Manuscript received: 22.02.2016;

More information

B. Loomis, D. Wiese, R. S. Nerem (1) P. L. Bender (2) P. N. A. M. Visser (3)

B. Loomis, D. Wiese, R. S. Nerem (1) P. L. Bender (2) P. N. A. M. Visser (3) Possible mission architectures for a GRACE follow-on mission including a study on upgraded instrumentation suites, and multiple satellite pairs in moderately-inclined orbits B. Loomis, D. Wiese, R. S.

More information

Relative Motion of Formation Flying with Elliptical Reference Orbit

Relative Motion of Formation Flying with Elliptical Reference Orbit Vol., No. 6, 13 Relative Motion of Formation Flying with Elliptical Reference Orbit Hany R Dwidar and Ashraf H. Owis Department of Astronomy, Space and Meteorology, Faculty of Science, Cairo University

More information

AN ANALYTICAL SOLUTION TO QUICK-RESPONSE COLLISION AVOIDANCE MANEUVERS IN LOW EARTH ORBIT

AN ANALYTICAL SOLUTION TO QUICK-RESPONSE COLLISION AVOIDANCE MANEUVERS IN LOW EARTH ORBIT AAS 16-366 AN ANALYTICAL SOLUTION TO QUICK-RESPONSE COLLISION AVOIDANCE MANEUVERS IN LOW EARTH ORBIT Jason A. Reiter * and David B. Spencer INTRODUCTION Collision avoidance maneuvers to prevent orbital

More information

MISSION PERFORMANCE MEASURES FOR SPACECRAFT FORMATION FLYING

MISSION PERFORMANCE MEASURES FOR SPACECRAFT FORMATION FLYING MISSION PERFORMANCE MEASURES FOR SPACECRAFT FORMATION FLYING Steven P. Hughes and Christopher D. Hall Aerospace and Ocean Engineering Virginia Polytechnic Institute and State University ABSTRACT Clusters

More information

Rendezvous Maneuvers of Multiple Spacecraft Using Differential Drag Under J 2 Perturbation

Rendezvous Maneuvers of Multiple Spacecraft Using Differential Drag Under J 2 Perturbation JOURNAL OF GUIDANCE, CONTROL, AND DYNAMICS Vol. 31, No. 6, November December 2008 Rendezvous Maneuvers of Multiple Spacecraft Using Differential Drag Under J 2 Perturbation R. Bevilacqua and M. Romano

More information

Differential Drag as a Means of Spacecraft Formation Control

Differential Drag as a Means of Spacecraft Formation Control Differential Drag as a Means of Spacecraft Formation Control BALAJI SHANKAR KUMAR ALFRED NG Canadian Space Agency KEISUKE YOSHIHARA Japan Aerospace Exploration Agency ANTON DE RUITER, Member, IEEE Canadian

More information

Onboard Maneuver Planning for the Autonomous Vision Approach Navigation and Target Identification (AVANTI) experiment within the DLR FireBird mission

Onboard Maneuver Planning for the Autonomous Vision Approach Navigation and Target Identification (AVANTI) experiment within the DLR FireBird mission Onboard Maneuver Planning for the Autonomous Vision Approach Navigation and Target Identification (AVANTI) experiment within the DLR FireBird mission G. Gaias, DLR/GSOC/Space Flight Technology Department

More information

Mission to Mars. MAE 598: Design Optimization Final Project. By: Trevor Slawson, Jenna Lynch, Adrian Maranon, and Matt Catlett

Mission to Mars. MAE 598: Design Optimization Final Project. By: Trevor Slawson, Jenna Lynch, Adrian Maranon, and Matt Catlett Mission to Mars MAE 598: Design Optimization Final Project By: Trevor Slawson, Jenna Lynch, Adrian Maranon, and Matt Catlett Motivation Manned missions beyond low Earth orbit have not occurred since Apollo

More information

A Space Debris Alert System for Aviation. US Patent pending Inventor: T. Sgobba - ESA Independent Safety Office

A Space Debris Alert System for Aviation. US Patent pending Inventor: T. Sgobba - ESA Independent Safety Office A Space Debris Alert System for Aviation US Patent pending Inventor: T. Sgobba - ESA Independent Safety Office Re-entry breakup basics Space systems in LEO reenter naturally at very shallow angle (

More information

Atmospheric Layers. Ionosphere. Exosphere. Thermosphere. Mesosphere. Stratosphere. Troposphere. mi (km) above sea level 250 (400) 50 (80) 30 (50)

Atmospheric Layers. Ionosphere. Exosphere. Thermosphere. Mesosphere. Stratosphere. Troposphere. mi (km) above sea level 250 (400) 50 (80) 30 (50) mi (km) above sea level Atmospheric Layers Exosphere 250 (400) Thermosphere Ionosphere 50 (80) Mesosphere Ozone Layer 30 (50) 7 (12) Stratosphere Troposphere Atmospheric Layers Earth s atmosphere is held

More information

Space Surveillance with Star Trackers. Part II: Orbit Estimation

Space Surveillance with Star Trackers. Part II: Orbit Estimation AAS -3 Space Surveillance with Star Trackers. Part II: Orbit Estimation Ossama Abdelkhalik, Daniele Mortari, and John L. Junkins Texas A&M University, College Station, Texas 7783-3 Abstract The problem

More information

SPACECRAFT NAVIGATION AND MISSION SIMULATION

SPACECRAFT NAVIGATION AND MISSION SIMULATION TianQin Space-borne gravitational wave detector SPACECRAFT NAVIGATION AND MISSION SIMULATION December 9, 2015 - Prepared by Viktor T. Toth A PERSPECTIVE Precision navigation End-to-end mission simulation

More information

Extending the Patched-Conic Approximation to the Restricted Four-Body Problem

Extending the Patched-Conic Approximation to the Restricted Four-Body Problem Monografías de la Real Academia de Ciencias de Zaragoza 3, 133 146, (6). Extending the Patched-Conic Approximation to the Restricted Four-Body Problem Thomas R. Reppert Department of Aerospace and Ocean

More information

IMPROVED DESIGN OF ON-ORBIT SEPARATION SCHEMES FOR FORMATION INITIALIZATION BASED ON J 2 PERTURBATION

IMPROVED DESIGN OF ON-ORBIT SEPARATION SCHEMES FOR FORMATION INITIALIZATION BASED ON J 2 PERTURBATION IAA-AAS-DyCoSS- IMPROVED DESIGN OF ON-ORBIT SEPARATION SCHEMES FOR FORMATION INITIALIZATION BASED ON J PERTURBATION Jiang Chao, * Wang Zhaokui, and Zhang Yulin INTRODUCTION Using one Multi-satellite Deployment

More information

NONLINEAR ANALYTICAL EQUATIONS OF RELATIVE MOTION ON J 2 -PERTURBED ECCENTRIC ORBITS

NONLINEAR ANALYTICAL EQUATIONS OF RELATIVE MOTION ON J 2 -PERTURBED ECCENTRIC ORBITS AAS 16-495 NONLINEAR ANALYTICAL EQUATIONS OF RELATIVE MOTION ON J 2 -PERTURBED ECCENTRIC ORBITS Bradley Kuiack and Steve Ulrich Future spacecraft formation flying missions will require accurate autonomous

More information

Massimiliano Vasile, Stefano Campagnola, Paolo Depascale, Stefano Pessina, Francesco Topputo

Massimiliano Vasile, Stefano Campagnola, Paolo Depascale, Stefano Pessina, Francesco Topputo A Toolbox for Preliminary Massimiliano Vasile, Stefano Campagnola, Paolo Depascale, Stefano Pessina, Francesco Topputo Mission Analysis and Design PAMSIT IMAGO ATOM-C EPIC Massimiliano Vasile, Stefano

More information

Distance of Mercury to the Sun or the Orbital Radius

Distance of Mercury to the Sun or the Orbital Radius Distance of Mercury to the Sun or the Orbital Radius The minimum distance from the Sun to Mercury is about 45866304 kilometers and the maximum distance is about 70006464 kilometers. Space Station One Day

More information

Module 4: Astronomy The Solar System Topic 3 Content: The Terrestrial Planets Notes Introduction

Module 4: Astronomy The Solar System Topic 3 Content: The Terrestrial Planets Notes Introduction Introduction The four planets closest to the Sun are called "the terrestrial planets." These inner planets are considered to be small and rocky. Although they are all rocky, their varying distances from

More information

Supplemental info for MCR : Change Science Orbit Period from 11 Days to 14 Days

Supplemental info for MCR : Change Science Orbit Period from 11 Days to 14 Days This document was reviewed and approved for export, see Juno-14-016. : Mission Engineer 6 May 2015 This document has been reviewed and determined not to contain export controlled technical data. Contents

More information

New Control Methodology for Nonlinear Systems and Its Application to Astrodynamics

New Control Methodology for Nonlinear Systems and Its Application to Astrodynamics New Control Methodology for Nonlinear Systems and Its Application to Astrodynamics Hancheol Cho, Ph.D. Marie-Curie COFUND Postdoctoral Fellow Space Structures and Systems Laboratory (S3L) Department of

More information

Autonomous optimal trajectory design employing convex optimization for powered descent on an asteroid

Autonomous optimal trajectory design employing convex optimization for powered descent on an asteroid Graduate Theses and Dissertations Iowa State University Capstones, Theses and Dissertations 2016 Autonomous optimal trajectory design employing convex optimization for powered descent on an asteroid Robin

More information

ABSTRACT. Nomenclature

ABSTRACT. Nomenclature ABSTRACT The behavior of two different models of gas-surface interactions is studied using the Direct Simulation Monte Carlo (DSMC) method. The DSMC calculations examine differences in predictions of aerodynamic

More information

Software Simulation of an Unmanned Vehicle Performing Relative Spacecraft Orbits

Software Simulation of an Unmanned Vehicle Performing Relative Spacecraft Orbits Software Simulation of an Unmanned Vehicle Performing Relative Spacecraft Orbits Christopher C. Romanelli Thesis submitted to the Faculty of the Virginia Polytechnic Institute and State University in partial

More information

NEW ADAPTIVE SLIDING MODE CONTROL AND RENDEZ-VOUS USING DIFFERENTIAL DRAG

NEW ADAPTIVE SLIDING MODE CONTROL AND RENDEZ-VOUS USING DIFFERENTIAL DRAG NEW ADAPTIVE SLIDING MODE CONTROL AND RENDEZ-VOUS USING DIFFERENTIAL DRAG Hancheol Cho Lamberto Dell Elce Gaëtan Kerschen Space Structures and Sstems Laborator (S3L) Universit of Liège, Belgium Contents

More information

New Worlds Observer Final Report Appendix J. Appendix J: Trajectory Design and Orbit Determination Lead Author: Karen Richon

New Worlds Observer Final Report Appendix J. Appendix J: Trajectory Design and Orbit Determination Lead Author: Karen Richon Appendix J: Trajectory Design and Orbit Determination Lead Author: Karen Richon The two NWO spacecraft will orbit about the libration point created by the Sun and Earth/Moon barycenter at the far side

More information

PW-Sat two years on orbit.

PW-Sat two years on orbit. 13th of February 2014 is the second anniversary of launch of the first polish student-made satellite PW-Sat. Currently Students' Space Association on Warsaw University of Technology is working on another

More information

Orekit at the U.S. Naval Research Laboratory. Evan Ward

Orekit at the U.S. Naval Research Laboratory. Evan Ward Orekit at the U.S. Naval Research Laboratory Evan Ward U.S. Naval Research Laboratory Astrodynamics and Navigation Section, Washington DC November 16, 2017 Outline Introduction Geolocation with Orekit

More information

GEO protected region: ISON capabilities to provide informational support for tasks of spacecraft flight safety and space debris removal

GEO protected region: ISON capabilities to provide informational support for tasks of spacecraft flight safety and space debris removal Russian Academy of Sciences Keldysh Institute of Applied Mathematics GEO protected region: ISON capabilities to provide informational support for tasks of spacecraft flight safety and space debris removal

More information

Goddard Space Flight Center

Goddard Space Flight Center 1 Solar Coronagraphs Observe off-disk coronal emissions from Sun. Dominant noise source: Diffraction of on-disk light around the occulter Vignetting on externally occulted coronagraphs Noise inversely

More information

BIRDY-T : Focus on propulsive aspects of an icubsat to small bodies of the solar system

BIRDY-T : Focus on propulsive aspects of an icubsat to small bodies of the solar system BIRDY-T : Focus on propulsive aspects of an icubsat to small bodies of the solar system Gary Quinsac, PhD student at PSL Supervisor: Benoît Mosser Co-supervisors: Boris Segret, Christophe Koppel icubesat,

More information

Mission Trajectory Design to a Nearby Asteroid

Mission Trajectory Design to a Nearby Asteroid Mission Trajectory Design to a Nearby Asteroid A project present to The Faculty of the Department of Aerospace Engineering San Jose State University in partial fulfillment of the requirements for the degree

More information

Newton s Legacy. 1- accelerate to break free of Earth. Rocket Science: How to send a spacecraft to Mars

Newton s Legacy. 1- accelerate to break free of Earth. Rocket Science: How to send a spacecraft to Mars Reading: today: web-based reading on satellite orbits; Chap. 3 Sec. 5 Chap. 7, Sect. 1, 2 (for next week) Exam 1: Tuesday, September 26, 6:45-8:00. Room assignments on course website ESSAY QUESTION Homework

More information

Lecture 23: Jupiter. Solar System. Jupiter s Orbit. The semi-major axis of Jupiter s orbit is a = 5.2 AU

Lecture 23: Jupiter. Solar System. Jupiter s Orbit. The semi-major axis of Jupiter s orbit is a = 5.2 AU Lecture 23: Jupiter Solar System Jupiter s Orbit The semi-major axis of Jupiter s orbit is a = 5.2 AU Jupiter Sun a Kepler s third law relates the semi-major axis to the orbital period 1 Jupiter s Orbit

More information

SELENE TRANSLUNAR TRAJECTORY AND LUNAR ORBIT INJECTION

SELENE TRANSLUNAR TRAJECTORY AND LUNAR ORBIT INJECTION SELENE TRANSLUNAR TRAJECTORY AND LUNAR ORBIT INJECTION Yasuihiro Kawakatsu (*1) Ken Nakajima (*2), Masahiro Ogasawara (*3), Yutaka Kaneko (*1), Yoshisada Takizawa (*1) (*1) National Space Development Agency

More information

Space Debris Re-entries and Aviation Safety

Space Debris Re-entries and Aviation Safety IAASS Space Debris Re-entries and Aviation Safety By Tommaso Sgobba IAASS President (iaass.president@gmail.com) International Association for the Advancement of Space Safety 1 Space debris as re-entry

More information

General Comments about the Atmospheres of Terrestrial Planets

General Comments about the Atmospheres of Terrestrial Planets General Comments about the Atmospheres of Terrestrial Planets Mercury Very little atmosphere Contents: vaporized micrometeorites, solar wind Sky is black Venus Very thick (10% density of water), dense

More information

Venus Express Aerobraking and End of Mission

Venus Express Aerobraking and End of Mission Venus Express Aerobraking and End of Mission Håkan Svedhem ESA/ESTEC Pericentre velocity vs Orbital Period Examples (VEX): Delta-V needed for Reduction of orbital period: 24h-18h 90m/s 18h-16h 42m/s 18h-12h

More information

Outline. Planetary Atmospheres. General Comments about the Atmospheres of Terrestrial Planets. General Comments, continued

Outline. Planetary Atmospheres. General Comments about the Atmospheres of Terrestrial Planets. General Comments, continued Outline Planetary Atmospheres Chapter 10 General comments about terrestrial planet atmospheres Atmospheric structure & the generic atmosphere Greenhouse effect Magnetosphere & the aurora Weather & climate

More information

AUTONOMOUS AND ROBUST RENDEZVOUS GUIDANCE ON ELLIPTICAL ORBIT SUBJECT TO J 2 PERTURBATION.

AUTONOMOUS AND ROBUST RENDEZVOUS GUIDANCE ON ELLIPTICAL ORBIT SUBJECT TO J 2 PERTURBATION. AUTONOMOUS AND ROBUST RENDEZVOUS GUIDANCE ON ELLIPTICAL ORBIT SUBJECT TO J 2 PERTURBATION Emmanuel GOGIBUS (1), Hervé CHARBONNEL (2), Patrick DELPY (3) (1) Astrium Space Transportation, 66 route de Verneuil,

More information

11.1 Survey of Spacecraft Propulsion Systems

11.1 Survey of Spacecraft Propulsion Systems 11.1 Survey of Spacecraft Propulsion Systems 11.1 Survey of Spacecraft Propulsion Systems In the progressing Space Age, spacecrafts such as satellites and space probes are the key to space exploration,

More information

The B-Plane Interplanetary Mission Design

The B-Plane Interplanetary Mission Design The B-Plane Interplanetary Mission Design Collin Bezrouk 2/11/2015 2/11/2015 1 Contents 1. Motivation for B-Plane Targeting 2. Deriving the B-Plane 3. Deriving Targetable B-Plane Elements 4. How to Target

More information

BravoSat: Optimizing the Delta-V Capability of a CubeSat Mission. with Novel Plasma Propulsion Technology ISSC 2013

BravoSat: Optimizing the Delta-V Capability of a CubeSat Mission. with Novel Plasma Propulsion Technology ISSC 2013 BravoSat: Optimizing the Delta-V Capability of a CubeSat Mission with Novel Plasma Propulsion Technology Sara Spangelo, NASA JPL, Caltech Benjamin Longmier, University of Michigan Interplanetary Small

More information

RELATIVE NAVIGATION FOR SATELLITES IN CLOSE PROXIMITY USING ANGLES-ONLY OBSERVATIONS

RELATIVE NAVIGATION FOR SATELLITES IN CLOSE PROXIMITY USING ANGLES-ONLY OBSERVATIONS (Preprint) AAS 12-202 RELATIVE NAVIGATION FOR SATELLITES IN CLOSE PROXIMITY USING ANGLES-ONLY OBSERVATIONS Hemanshu Patel 1, T. Alan Lovell 2, Ryan Russell 3, Andrew Sinclair 4 "Relative navigation using

More information

The Inner Planets. Chapter 3 Lesson 1. Pages Workbook pages 51-52

The Inner Planets. Chapter 3 Lesson 1. Pages Workbook pages 51-52 The Inner Planets Chapter 3 Lesson 1 Pages 152-159 Workbook pages 51-52 Create the Foldable on pg 159 The solar The planets system The four inner planets Compare and Contrast Question What are planets?

More information

ASTRIUM. Interplanetary Path Early Design Tools at ASTRIUM Space Transportation. Nathalie DELATTRE ASTRIUM Space Transportation.

ASTRIUM. Interplanetary Path Early Design Tools at ASTRIUM Space Transportation. Nathalie DELATTRE ASTRIUM Space Transportation. Interplanetary Path Early Design Tools at Space Transportation Nathalie DELATTRE Space Transportation Page 1 Interplanetary missions Prime approach: -ST has developed tools for all phases Launch from Earth

More information

Toshinori Kuwahara*, Yoshihiro Tomioka, Yuta Tanabe, Masato Fukuyama, Yuji Sakamoto, Kazuya Yoshida, Tohoku University, Japan

Toshinori Kuwahara*, Yoshihiro Tomioka, Yuta Tanabe, Masato Fukuyama, Yuji Sakamoto, Kazuya Yoshida, Tohoku University, Japan Toshinori Kuwahara*, Yoshihiro Tomioka, Yuta Tanabe, Masato Fukuyama, Yuji Sakamoto, Kazuya Yoshida, Tohoku University, Japan The 3 rd Nano-Satellite Symposium Micro/Nano Satellite & Debris Issues December

More information

Orbit Design Marcelo Suárez. 6th Science Meeting; Seattle, WA, USA July 2010

Orbit Design Marcelo Suárez. 6th Science Meeting; Seattle, WA, USA July 2010 Orbit Design Marcelo Suárez Orbit Design Requirements The following Science Requirements provided drivers for Orbit Design: Global Coverage: the entire extent (100%) of the ice-free ocean surface to at

More information

Autonomous Vision Based Detection of Non-stellar Objects Flying in formation with Camera Point of View

Autonomous Vision Based Detection of Non-stellar Objects Flying in formation with Camera Point of View Autonomous Vision Based Detection of Non-stellar Objects Flying in formation with Camera Point of View SFFMT 213 München May 31 st 213 Mathias Benn, As.Prof, PhD John L. Jørgensen, Prof. DTU Space Overview

More information

THE DEVELOPMENT OF HIGH FIDELITY LINEARIZED J 2 MODELS FOR SATELLITE FORMATION FLYING CONTROL

THE DEVELOPMENT OF HIGH FIDELITY LINEARIZED J 2 MODELS FOR SATELLITE FORMATION FLYING CONTROL AAS 4-16 THE DEVELOPMENT OF HIGH FIDELITY LINEARIZED J MODELS FOR SATELLITE FORMATION FLYING CONTROL INTRODUCTION Jennifer A. Roberts * and Peter C. E. Roberts The inclusion of the linearized J effect

More information

Robotic Mobility Above the Surface

Robotic Mobility Above the Surface Free Space Relative Orbital Motion Airless Major Bodies (moons) 1 2016 David L. Akin - All rights reserved http://spacecraft.ssl.umd.edu Propulsive Motion in Free Space Basic motion governed by Newton

More information

Mars Sample Return Mission

Mars Sample Return Mission Mars Sample Return Mission Ryan Supler Saylor.org: SSE101 MSRM Project April 15, 2014 2 Table of Contents The Scoping Elements of the Mars Sample Return Mission page 3 The High-Level Concept of Operations

More information

Initial Trajectory and Atmospheric Effects

Initial Trajectory and Atmospheric Effects Initial Trajectory and Atmospheric Effects G. Flanagan Alna Space Program July 13, 2011 Introduction A major consideration for an earth-based accelerator is atmospheric drag. Drag loses mean that the gun

More information

Discrete-Time Optimization and Safe-Trajectory. Generation for Satellite Formation Flying and. Proximity Operations

Discrete-Time Optimization and Safe-Trajectory. Generation for Satellite Formation Flying and. Proximity Operations Discrete-Time Optimization and Safe-Trajectory Generation for Satellite Formation Flying and Proximity Operations Kristen Tetreault 1, Ian Elliott 2, Shane D. Ross 3, and Jonathan Black 4 Virginia Polytechnic

More information

Aerobraking A mission enabling and fuel saving technique for orbit changes - Venus Express and ExoMars TGO. Håkan Svedhem ESA/ESTEC

Aerobraking A mission enabling and fuel saving technique for orbit changes - Venus Express and ExoMars TGO. Håkan Svedhem ESA/ESTEC ILEWG Aerobraking A mission enabling and fuel saving technique for orbit changes - Venus Express and ExoMars TGO Håkan Svedhem ESA/ESTEC ILEWG Earth Venus Trajectory 2 ILEWG Reducing Apocentre altitude

More information

Quasi-Satellite Orbits around Deimos and Phobos motivated by the DePhine Mission Proposal

Quasi-Satellite Orbits around Deimos and Phobos motivated by the DePhine Mission Proposal Quasi-Satellite Orbits around Deimos and Phobos motivated by the DePhine Mission Proposal By Sofya SPIRIDONOVA, 1) Kai WICKHUSEN, 2) Ralph KAHLE 1) and Jürgen OBERST 2) 1) German Space Operations Center,

More information

Spacecraft De-Orbit Point Targeting using Aerodynamic Drag

Spacecraft De-Orbit Point Targeting using Aerodynamic Drag AIAA SciTech Forum 9-13 January 2017, Grapevine, Texas AIAA Guidance, Navigation, and Control Conference AIAA 2017-1268 Spacecraft De-Orbit Point Targeting using Aerodynamic Drag Sanny R. Omar 1 and Riccardo

More information

ATTITUDE CONTROL MECHANIZATION TO DE-ORBIT SATELLITES USING SOLAR SAILS

ATTITUDE CONTROL MECHANIZATION TO DE-ORBIT SATELLITES USING SOLAR SAILS IAA-AAS-DyCoSS2-14-07-02 ATTITUDE CONTROL MECHANIZATION TO DE-ORBIT SATELLITES USING SOLAR SAILS Ozan Tekinalp, * Omer Atas INTRODUCTION Utilization of solar sails for the de-orbiting of satellites is

More information

Mars Update. Presented by NASA/JPL Solar System Educator Don W. Brown

Mars Update. Presented by NASA/JPL Solar System Educator Don W. Brown Mars Update Presented by NASA/JPL Solar System Educator Don W. Brown http://www.wired.com/wiredscience/2010/01/gallery-mars/6/ Mariner Mars Climate Orbiter Mars Exploration Rovers Mars Global Surveyor

More information

Small Entry Probe Trajectories for Mars

Small Entry Probe Trajectories for Mars CubeSat (re-)entry can mean burning up in the atmosphere Here, we discuss surviving atmospheric entry We must model & understand flight dynamics, aerodynamics, heating Motivation for CubeSat entry Support

More information

Previous Lecture. Orbital maneuvers: general framework. Single-impulse maneuver: compatibility conditions

Previous Lecture. Orbital maneuvers: general framework. Single-impulse maneuver: compatibility conditions 2 / 48 Previous Lecture Orbital maneuvers: general framework Single-impulse maneuver: compatibility conditions closed form expression for the impulsive velocity vector magnitude interpretation coplanar

More information

Planetary Protection at ESA Issues & Status

Planetary Protection at ESA Issues & Status Planetary Protection at ESA Issues & Status Gerhard Kminek Planetary Protection Officer, ESA NASA Planetary Protection Subcommittee Meeting 12-13 November 2013, GSFC Selected Missions BepiColombo Launch

More information

Past and Future Climate of Thermospheric Density: Solar and Anthropogenic Influences

Past and Future Climate of Thermospheric Density: Solar and Anthropogenic Influences Past and Future Climate of Thermospheric Density: Solar and Anthropogenic Influences Thermosphere energy balance Thermosphere climate from satellite drag Attribution of 2008 solar minimum behavior Scenarios

More information

AST111, Lecture 1b. Measurements of bodies in the solar system (overview continued) Orbital elements

AST111, Lecture 1b. Measurements of bodies in the solar system (overview continued) Orbital elements AST111, Lecture 1b Measurements of bodies in the solar system (overview continued) Orbital elements Planetary properties (continued): Measuring Mass The orbital period of a moon about a planet depends

More information

Enhanced GPS Accuracy using Lunar Transponders

Enhanced GPS Accuracy using Lunar Transponders Enhanced GPS Accuracy using Lunar Transponders G. Konesky SGK NanoStructures, Inc. LEAG - ICEUM - SSR Port Canaveral, FL Oct. 28-31, 2008 GPS Broadcast Ephemeris Error Nov. 1, 1997 Warren, 2002 Warren,

More information

SPACE DEBRIS MITIGATION TECHNOLOGIES

SPACE DEBRIS MITIGATION TECHNOLOGIES SPACE DEBRIS MITIGATION TECHNOLOGIES Rob Hoyt Tethers Unlimited, Inc. The orbital debris population and its potential for continued rapid growth presents a significant threat to DoD, NASA, commercial,

More information

Collision Risk Assessment for Spacecraft with CASS

Collision Risk Assessment for Spacecraft with CASS Collision Risk Assessment for Spacecraft with CASS Ma Chaowei 2011, 17-18 Oct 2011 Beijing Institute of Tracking and Telecommunications Technology Ma Chaowei 2 Contents Introduction Basic Information of

More information

DEFLECTING HAZARDOUS ASTEROIDS FROM COLLISION WITH THE EARTH BY USING SMALL ASTEROIDS

DEFLECTING HAZARDOUS ASTEROIDS FROM COLLISION WITH THE EARTH BY USING SMALL ASTEROIDS DEFLECTING HAZARDOUS ASTEROIDS FROM COLLISION WITH THE EARTH BY USING SMALL ASTEROIDS N. Eismont (1), M. Boyarsky (1), A. Ledkov (1), B.Shustov (2), R. Nazirov (1), D. Dunham (3) and K. Fedyaev (1) (1)

More information

MARS. The Red Planet

MARS. The Red Planet MARS The Red Planet About the Planet Common Name: Mars Mythological Name(s): - Greek: Ares - Roman: Mars Mars is named after the Roman God of War A few Pictures... Distance, Size, and Gravity Compared

More information

Inner Planets (Part II)

Inner Planets (Part II) Inner Planets (Part II) Sept. 18, 2002 1) Atmospheres 2) Greenhouse Effect 3) Mercury 4) Venus 5) Mars 6) Moon Announcements Due to technical difficulties, Monday s quiz doesn t count An extra credit problem

More information

Autonomous Trajectory Planning by Convex Optimization

Autonomous Trajectory Planning by Convex Optimization Graduate Theses and Dissertations Graduate College 213 Autonomous Trajectory Planning by Convex Optimization Xinfu Liu Iowa State University Follow this and additional works at: http://lib.dr.iastate.edu/etd

More information

Deorbiting Upper-Stages in LEO at EOM using Solar Sails

Deorbiting Upper-Stages in LEO at EOM using Solar Sails Deorbiting Upper-Stages in LEO at EOM using Solar Sails Alexandru IONEL* *Corresponding author INCAS National Institute for Aerospace Research Elie Carafoli, B-dul Iuliu Maniu 220, Bucharest 061126, Romania,

More information

Study of the decay time of a CubeSat type satellite considering perturbations due to the Earth's oblateness and atmospheric drag

Study of the decay time of a CubeSat type satellite considering perturbations due to the Earth's oblateness and atmospheric drag Journal of Physics: Conference Series PAPER OPEN ACCESS Study of the decay time of a CubeSat type satellite considering perturbations due to the Earth's oblateness and atmospheric drag To cite this article:

More information

ADVANCED NAVIGATION STRATEGIES FOR AN ASTEROID SAMPLE RETURN MISSION

ADVANCED NAVIGATION STRATEGIES FOR AN ASTEROID SAMPLE RETURN MISSION AAS 11-499 ADVANCED NAVIGATION STRATEGIES FOR AN ASTEROID SAMPLE RETURN MISSION J. Bauman,* K. Getzandanner, B. Williams,* K. Williams* The proximity operations phases of a sample return mission to an

More information

Introduction to Satellite Orbits

Introduction to Satellite Orbits Introduction to Satellite Orbits Dinesh Manandhar Center for Spatial Information Science The University of Tokyo Contact Information: dinesh@iis.u-tokyo.ac.jp Slide : 1 Basics of Satellite Orbits The speed

More information

Modeling, Dynamics and Control of Spacecraft Relative Motion in a Perturbed Keplerian Orbit

Modeling, Dynamics and Control of Spacecraft Relative Motion in a Perturbed Keplerian Orbit Paper Int l J. of Aeronautical & Space Sci. 16(1), 77 88 (2015) http://dx.doi.org/10.5139/ijass.2015.16.1.77 Modeling, Dynamics and Control of Spacecraft Relative Motion in a Perturbed Keplerian Orbit

More information

How Small Can a Launch Vehicle Be?

How Small Can a Launch Vehicle Be? UCRL-CONF-213232 LAWRENCE LIVERMORE NATIONAL LABORATORY How Small Can a Launch Vehicle Be? John C. Whitehead July 10, 2005 41 st AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit Tucson, AZ Paper

More information

Measuring Global Temperatures: Satellites or Thermometers?

Measuring Global Temperatures: Satellites or Thermometers? Measuring Global Temperatures: Satellites or Thermometers? January 26, 2016 by Dr. Roy Spencer, http://www.cfact.org/2016/01/26/measuring-global-temperatures-satellites-orthermometers/ The University of

More information