SPACE DEBRIS REMOVAL

Similar documents
INTER-AGENCY SPACE DEBRIS COORDINATION COMMITTEE (IADC) SPACE DEBRIS ISSUES IN THE GEOSTATIONARY ORBIT AND THE GEOSTATIONARY TRANSFER ORBITS

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

Propellantless deorbiting of space debris by bare electrodynamic tethers

End of Life Re-orbiting The Meteosat-5 Experience

Prospects for the use of nuclear power sources in outer space. Working document submitted by the Russian Federation

USA Space Debris Environment, Operations, and Modeling Updates

Satellite Orbital Maneuvers and Transfers. Dr Ugur GUVEN

Solid Propellant Autonomous DE-Orbit System [SPADES]

Level 3 Physics, 2018

CHAPTER 3 PERFORMANCE

The Launch of Gorizont 45 on the First Proton K /Breeze M

Systems Engineering in Venus Satellite

Ball Aerospace & Technologies Corp. & L Garde Inc.

Learning Lab Seeing the World through Satellites Eyes

Orbital Debris Observation via Laser Illuminated Optical Measurement Techniques

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

A Regional Microsatellite Constellation with Electric Propulsion In Support of Tuscan Agriculture

SOLVING THE INTERNATIONAL SPACE STATION (ISS) MOTION CONTROL LONG-TERM PLANNING PROBLEM

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

Successful Demonstration for Upper Stage Controlled Re-entry Experiment by H-IIB Launch Vehicle

GUIDANCE, NAVIGATION, AND CONTROL TECHNIQUES AND TECHNOLOGIES FOR ACTIVE DEBRIS REMOVAL

SLR-based orbit determination and orbit prediction of space debris objects

1. (a) Describe the difference between over-expanded, under-expanded and ideallyexpanded

MAE 180A: Spacecraft Guidance I, Summer 2009 Homework 4 Due Thursday, July 30.

Technology of Rocket

FEDERAL SPACE AGENCY OF RUSSIA ACTIVITY OF RUSSIAN FEDERATION ON SPACE DEBRIS PROBLEM

LAUNCH SYSTEMS. Col. John Keesee. 5 September 2003

Optimal Gravity Assisted Orbit Insertion for Europa Orbiter Mission

ESSE Payload Design. 1.2 Introduction to Space Missions

9.2 Worksheet #3 - Circular and Satellite Motion

Problem A: Solar Sailing to Mars

Optimization of Orbital Transfer of Electrodynamic Tether Satellite by Nonlinear Programming

IMPACT OF SPACE DEBRIS MITIGATION REQUIREMENTS ON THE MISSION DESIGN OF ESA SPACECRAFT

Space Debris Activities in India

CHAPTER 3 PERFORMANCE

CHOICE OF A SUITABLE TARGET FOR DEVELOPING PROPOSALS FOR AN ADR FLIGHT DEMONSTRATION EXPERIMENT

IAC-16.A Jason A. Reiter a *, David B. Spencer b

Science in the news Voyager s 11 billion mile journey

The driver then accelerates the car to 23 m/s in 4 seconds. Use the equation in the box to calculate the acceleration of the car.

Space Travel on a Shoestring: CubeSat Beyond LEO

RADIATION OPTIMUM SOLAR-ELECTRIC-PROPULSION TRANSFER FROM GTO TO GEO

Space Debris Assessment for USA-193

The Kerbal Space Program

USA Space Debris Environment and Operational Updates

The Inter-Agency Space Debris Coordination Committee (IADC)

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

Solid Propellant Autonomous DE-Orbit System [SPADES] Co-authors: T. Soares J. Huesing A. Cotuna I. Carnelli L. Innocenti

Marlene H. Dortch Secretary, Federal Communications Commission th Street, S.W. Washington, D.C

Figure 1. View of ALSAT-2A spacecraft

All questions are of equal value. No marks are subtracted for wrong answers.

Some Questions We ll Address Today

CHAPTER 3 PERFORMANCE

System and Concurrent Engineering for the e.deorbit Mission Assessment Studies Robin Biesbroek Jakob Hüsing Andrew Wolahan

ASTRIUM. Minimum-time problem resolution under constraints for low-thrust stage trajectory computation. Nathalie DELATTRE ASTRIUM Space Transportation

SURVEY OF THE ELECTRIC SOLAR WIND SAIL: THE FASTEST MAN-MADE DEVICE EVER BUILT

A Passive De-orbiting Strategy for High Altitude CubeSat Missions using a Deployable Reflective Balloon

Abstract of: NEO - MIPA. Near-Earth Object Hazard Mitigation Publication Analysis

Physics 201 Quiz 1. Jan 14, 2013

Launch strategy for Indian lunar mission and precision injection to the Moon using genetic algorithm

Space Debris Reentry Hazards

THE TRAJECTORY CONTROL STRATEGIES FOR AKATSUKI RE-INSERTION INTO THE VENUS ORBIT

Attitude Control Method of Spin-Stabilized Satellite Base on Equiangular Precession

Research Article Generalized Guidance Scheme for Low-Thrust Orbit Transfer

Proton Launch System Mission Planner s Guide APPENDIX F. Proton Launch System Options and Enhancements

EUROSTAR 3000 INCLINED ORBIT MISSION : LIFETIME OPTIMISATION IN CASE OF INJECTION WITH A LOW INCLINATION

USA Space Debris Environment, Operations, and Policy Updates

COUPLED OPTIMIZATION OF LAUNCHER AND ALL-ELECTRIC SATELLITE TRAJECTORIES

4.8 Space Research and Exploration. Getting Into Space

ROCSAT-3 Constellation Mission

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

Deorbiting Upper-Stages in LEO at EOM using Solar Sails

2. To study circular motion, two students use the hand-held device shown above, which consists of a rod on which a spring scale is attached.

DEBRIS IMPACT ON LOW EARTH ORBIT SPACE MISSION

Proton Launch System Mission Planner s Guide SECTION 2. LV Performance

ENAE 483/788D MIDTERM FALL, 2018 NAME: a 3 = a = 42970] 1. So after one sol, the subspacecraft point would have gone 88773

Sail-Assisted End-of-Life Disposal of High-LEO Satellites

Information furnished in conformity with the Convention on Registration of Objects Launched into Outer Space

Electromagnetic Tethers as Deorbit Devices - Numerical Simulation of Upper-Stage Deorbit Efficiency

Responsive Imaging Constellations for Support of Geographically Dispersed Theaters

Laser de-spin maneuver for an active debris removal mission - a realistic scenario for Envisat

Traveling Into Space. Use Target Reading Skills. How Do Rockets Work? Building Vocabulary

ATTITUDE CONTROL MECHANIZATION TO DE-ORBIT SATELLITES USING SOLAR SAILS

Universal Space Vehicle Design Concept to Defend the Earth against Asteroidal-Cometary Danger

The Satellite Sweeper Approach for the Solution of the Space Debris Problem

Using the International Space Station as an Engineering Technology Research Laboratory for Space Based Telescopes

AA 528 Spacecraft Dynamics and Control. Mehran Mesbahi Aeronautics & Astronautics Winter 2017 University of Washington

on space debris objects obtained by the

STUDY THE SPACE DEBRIS IMPACT IN THE EARLY STAGES OF THE NANO-SATELLITE DESIGN

Orbital Debris Mitigation

A/AC.105/C.2/2015/CRP.18

Rapid De-Orbit of LEO Space Vehicles Using Towed Rigidizable Inflatable Structure (TRIS) Technology: Concept and Feasibility Assessment

AP Physics C Summer Assignment Kinematics

SELENE TRANSLUNAR TRAJECTORY AND LUNAR ORBIT INJECTION

Preliminary Design Review: Loads, Structures, and Mechanisms. Michael Cunningham, Shimon Gewirtz, Rajesh Yalamanchili, Thomas Noyes

How Small Can a Launch Vehicle Be?

Orbit Evolution of the Swarm Mission Detlef Sieg

The Orbit Control of ERS-1 and ERS-2 for a Very Accurate Tandem Configuration

Spacecraft motion and attitude control in the high elliptic orbit

Thank you for your purchase!

12.3 Exploring Space: Past, Present and Future

Transcription:

M.K. Yangel Yuzhnoye State Design Office Ukraine SPACE DEBRIS REMOVAL The Fiftieth Session of the Scientific and Technical Subcommittee of the Committee on the Peaceful Uses of Outer Space Vienna International Centre, Vienna, Austria 11-22 February 2013 E-mail: info@yuzhnoye.com 1

STATEMENT OF SPACE DEBRIS REMOVAL PROBLEM The research «Space Debris Environment Remediation», conducted by International Academy of Astronautics in 2011, contains review of various space debris removal technologies and methodologies, and analysis of their applicability to different debris objects and their types of orbits. Our view of the problem of cleaning up the space environment is as follows. Space debris removal problem is complex, i.e. it includes a range of tasks: ü Identification of space debris objects and their initial orbit parameters determination. ü Prediction of space debris objects motion parameters. ü Interception satellite optimal trajectory selection. ü Ensuring the interception satellite s guidance and its rendezvous with a space debris object. ü Ensuring an effective impact on an object that will guarantee its deorbiting. 2

CHALLENGES IN SOLVING SPACE DEBRIS REMOVAL PROBLEM Challenges in solving indicated space debris removal tasks include the following: ü Because space debris objects do not have any tools for measuring their motion parameters, this task can be solved only by means (ground- or space-based) of location (radio- or optical). ü Space debris objects vary in mass and size, i.e. the use of one device for effective removal of any objects seems to be impossible. ü Space debris objects hold great amounts of energy (34 57 MJ/kg depending on orbit altitude), and for effective space debris removal it should be spent at least to 1% of this energy. ü Usually, space debris objects spin chaotically, which makes it difficult to mount deorbiting devices on them. ü Trajectories of most space debris objects lie in the region of functioning spacecraft, i.e. an impact must be applied to a specific space debris object and must not influence the functioning spacecraft. ü Large space debris objects can be fragmented into smaller pieces from a strong mechanical impact, which in most cases leads to growth of space debris. 3

SPACE DEBRIS REMOVAL PROBLEM SOLVING CONDITIONS Effective solution to indicated space debris removal tasks includes next: ü Use of space-based means of location for detecting and measuring the motion parameters of space debris objects. Today, for objects larger than 0.1 m it s done by ground-based means. ü Forecast precision of space debris objects motion parameters should be 1 100 m (depending on an employed space debris removal technology) at least on the interval of one orbit pass (~100 minutes for LEO objects). Methods that are used today have forecast precision of functioning spacecraft coordinates ~1 km on the interval of twenty-four hours (i.e. ~70 m on the interval of one orbit pass). ü Trajectory of an interception satellite, despite a type of used space debris removal technology, should ensure it can deorbit as many objects as possible, and does not influence the functioning spacecraft. ü Guidance of an interception satellite and its rendezvous with a space debris object should be done by means of location and high maneuverability propulsion system. ü Criteria of impact effectiveness on a space debris object can be drawn from its deorbiting duration. 4

EFFECTIVE SPACE DEBRIS REMOVAL SYSTEM In our opinion, most effective impact on small, so as on large space debris objects (in terms of duration and cost of removal of one kilogram of debris), will be from smashing one with another object. By estimate, for fast (in just a few orbit passes) deorbiting of 1,000-kg space debris object from a 600 900-km altitude it s sufficient to smash it with an orbiting in opposite direction 10 15-kg object (a Kicker Load). The KL deorbits as well. In realization of this technology, an acute problem that has to be found a solution to is to make sure a space debris object does not fragment from the impact of a kicker load, or in case it does, all the fragments will deorbit as well. Conducted in YSDO research shows this problem can be solved by using KL deformable structure of large size that will stall space debris object fragments after its collision. 5

PRINCIPLES OF KICKER LOADS SYSTEM OPERATION The following space debris removal system for specific region, e.g. sun-synchronous orbits with constrained parameters, seems to be effective: - altitude h min toh max ; - inclination i min toi max ; - local solar time in ascending node t Wmin tot Wmax. Before launching an interception satellite for cleaning up a specific range of orbits, a list of due to removal space debris objects has to be specified, and preliminary forecast of their trajectories carried out. An interception satellite with a set of kicker loads is launched into an orbit with a h max - altitude, (180 -i max )-inclination and (12 h +t Wmax )-local solar time in ascending node. 6

PRINCIPLES OF KICKER LOADS SYSTEM OPERATION Due to long surveillance (with the help of ground-based means, and perhaps, interception satellite on-board means of location) forecast precision of an object s coordinates is brought to a few meters. It s sufficient to drive to this level of accuracy the forecast of just altitude and orbit binormal (trajectories tube radius) of a space debris object. At the same time, ground control center (GCC) determines and predicts the interception satellite s motion parameters. On a basis of motion parameters forecast for a space debris object and the interceptor, GCC generates control commands and transmits them to the satellite. 7

PRINCIPLES OF KICKER LOADS SYSTEM OPERATION At a specified moment of time (less than an orbit pass) the interceptor using its high maneuverability propulsion system moves onto an object s trajectory but of opposite direction, and leaves there a kicker load. 8

PRINCIPLES OF KICKER LOADS SYSTEM OPERATION After a KL separates on a rendezvous trajectory, the interceptor moves to another, detects an approaching space debris object and takes it under surveillance. A KL automatically unfolds to a necessary extent (10 20 m) and awaits a space debris object. If the need arises, trajectory corrections of a KL (up-down, left-right) can be performed with mounted on it micromotors via remote commands from the satellite. 9

PRINCIPLES OF KICKER LOADS SYSTEM OPERATION When a space debris object collides against a sequence of deformable surfaces of a KL, a step decrease of an object s velocity and its fragmentation into separate pieces that stay inside the KL take place. The interceptor conducts surveillance over the process of a KL and space debris object colliding together with its camera for transmitting the reportage to GCC. 10

PRINCIPLES OF KICKER LOADS SYSTEM OPERATION As a result of impulse loss, a space debris object (its fragments) along with a KL moves to an orbit that leads to deorbitation, and the satellite embarks on a process of deorbiting next object. After cleaning up orbits of h max the interception satellite transfers itself into lower orbits. In this fashion, the interceptor cleans up the specified range of orbits region by region until it gets to h min. After mission is completed, it delivers itself to a graveyard orbit. 11

OPERATION SCENARIOS OF KICKER LOADS SYSTEM There s an option of space debris object removal of longer duration. In this case, the interception satellite leaves a KL not on a rendezvous trajectory, but on that of the space debris object. 1. On a basis of motion parameters forecast for a space debris object and the interceptor, GCC generates control commands and transmits them to the satellite. 2. At a specified moment of time the interceptor using its high maneuverability propulsion system moves onto an object s trajectory and attaches to an object a deorbiting device. 12

OPERATION SCENARIOS OF KICKER LOADS SYSTEM Guidance of a KL is carried out by remote commands from the satellite that conducts surveillance over the space debris object. 3. A deorbiting device is attached to a space debris object. The interceptor transfers itself onto the trajectory of another object. 4. A deorbiting device (e.g. a drag augmentation inflatable structure) unfolds on an object. 13

INFLATABLE DRAG DEVICES DESIGNS The covers of balls and inflatable structures are made of light, thin, and strong material. A whole ball-shaped shell A group of several combined whole ballshaped shells 14

INFLATABLE DRAG DEVICES DESIGNS Structure designs that increase survivability of an inflatable drag system when colliding with small (less than 10 cm) debris. A frame ball-shaped structure A segmental ball-shaped structure 15

DEORBITING SCENARIOS OF LV LIQUID-PROPELLANT UPPER STAGES Removal of LV upper liquid-propellant stages after delivery/separation of spacecraft can be carried out by mounted on propellant tanks reverse thrust nozzles with membranes. After propulsion system is shut down, membranes open and the pressurant from tanks begin to run through the nozzles, decelerating and twisting the stage around its longitudinal axis for ensuring the oriented travel. To speed up the drag process of a stage the residual propellant in fuel tanks can be gradually afterburned. 16

PROPOSALS ON SYSTEMS DEVELOPMENT Development proposals of: a satellite system for effective space debris removal; an inflatable drag system that decreases a space debris object s orbit; a gas-dynamic removal system of LV upper liquid-propellant stages. Development process of a satellite system will include: ü Examination of principles of interception satellite operation and analysis of its various designs. ü Computation of key parameters of an interceptor and KL. ü Mathematical and physical simulation of the KL and space debris object collision process. ü Elaboration of design and development documentation. ü Manufacturing and testing of KL samples. ü Manufacturing of an interception satellite demonstration unit. Project execution phases: ü Conceptual design. ü Design and development documentation. ü Experimental maturation. ü Spacecraft demonstration unit manufacturing. 17

PROPOSALS ON SYSTEMS DEVELOPMENT Development process of an inflatable drag system will include: ü Selection of material and source of pressurant for the shell. ü Computation of key parameters of an inflatable drag system. ü Development of a pressurant control system. ü Development of a storage system for inflatable devices inside the spacecraft and a system responsible for attaching them to space debris objects. ü Elaboration of design and development documentation. ü Manufacturing and testing of inflatable drag system samples. ü Manufacturing of inflatable drag system demonstration units. Project execution phases: ü Conceptual design. ü Draft design. ü Engineering design. ü Experimental maturation and clarification of development documentation. ü Inflatable drag system demonstration units manufacturing. 18

PROPOSALS ON SYSTEMS DEVELOPMENT Development process of a gas-dynamic removal system will include : ü Conceptual scheme development of a depressurization system. ü Computation of key parameters of a depressurization system. ü Development of an afterburn system of residual propellant from either oxidizer or fuel tanks. ü Elaboration of design and development documentation. ü Manufacturing and testing of gas-dynamic removal system samples. ü Manufacturing of gas-dynamic removal system demonstration units. Project execution phases : ü Conceptual design. ü Draft design. ü Engineering design. ü Experimental maturation and clarification of development documentation. ü Manufacturing of gas-dynamic removal system demonstration units on LV. 19

CONTACT INFORMATION Alexander Degtyarev General Designer General Director of Yuzhnoye State Design Office Dnepropetrovsk city, 3, Krivorozhskaya street 49008, Ukraine Phone: +380 56 242 00 22 Fax: +380 56 770 01 25 Е-mail: space@yuzhnoye.com 20