ACCURACY ASSESSMENT OF GEOSTATIONARY-EARTH-ORBIT WITH SIMPLIFIED PERTURBATIONS MODELS

Similar documents
Improving LEO prediction precision with TLEs

Experimental Analysis of Low Earth Orbit Satellites due to Atmospheric Perturbations

Astrodynamics (AERO0024)

Calculation of Earth s Dynamic Ellipticity from GOCE Orbit Simulation Data

MULTI PURPOSE MISSION ANALYSIS DEVELOPMENT FRAMEWORK MUPUMA

APPENDIX TLE TWO-LINE ELEMENT TRACKING

Increasing the Accuracy of Orbital Position Information from NORAD SGP4 Using Intermittent GPS Readings

PW-Sat two years on orbit.

IMPROVED ORBITAL DEBRIS TRAJECTORY ESTIMATION BASED ON SEQUENTIAL TLE PROCESSING ABSTRACT

Section 13. Orbit Perturbation. Orbit Perturbation. Atmospheric Drag. Orbit Lifetime

Keplerian Elements Tutorial

Astrodynamics (AERO0024)

ORBIT DESIGN AND SIMULATION FOR KUFASAT NANO- SATELLITE

A Fast Method for Embattling Optimization of Ground-Based Radar Surveillance Network

ORBITAL DECAY PREDICTION AND SPACE DEBRIS IMPACT ON NANO-SATELLITES

AIR FORCE INSTITUTE OF TECHNOLOGY

Polarization Tracking Study of Earth Station in Satellite Communications

Astrodynamics (AERO0024)

Fundamentals of Astrodynamics and Applications

8 Sateph User s manual

An Optical Survey for Space Debris on Highly Eccentric MEO Orbits

MAHALAKSHMI ENGINEERING COLLEGE-TRICHY QUESTION BANK UNIT I PART A

Astrodynamics (AERO0024)

Improvement of Orbits of Geostationary Satellites from Observations Over a Time Interval of Days

Creating Satellite Orbits

Celestial Mechanics and Satellite Orbits

Figure 1. View of ALSAT-2A spacecraft

MODELLING OF PERTURBATIONS FOR PRECISE ORBIT DETERMINATION

Lunisolar Secular Resonances

A Survey and Performance Analysis of Orbit Propagators for LEO, GEO, and Highly Elliptical Orbits

Fundamentals of Satellite technology

Lecture 2c: Satellite Orbits

GPS Results for the Radio Aurora Explorer II CubeSat Mission

Analytical Method for Space Debris propagation under perturbations in the geostationary ring

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

Software and hardware implements for tracking low earth orbit (LEO) satellites

MAE 180A: Spacecraft Guidance I, Summer 2009 Homework 2 Due Tuesday, July 14, in class.

COVARIANCE DETERMINATION, PROPAGATION AND INTERPOLATION TECHNIQUES FOR SPACE SURVEILLANCE. European Space Surveillance Conference 7-9 June 2011

2. The line joining the planet to the Sun sweeps out equal areas in equal times.

SCIENCE & TECHNOLOGY

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

Long-Term Evolution of High Earth Orbits: Effects of Direct Solar Radiation Pressure and Comparison of Trajectory Propagators

Chapter 2: Orbits and Launching Methods

INTEROPERABILITY AND STANDARDS ACROSS THE ENTIRE SPACE ENTERPRISE. GSAW 2007 Manhattan Beach, CA March 2007

On Sun-Synchronous Orbits and Associated Constellations

Satellite Communications

EasyChair Preprint. Retrograde GEO Orbit Design Method Based on Lunar Gravity Assist for Spacecraft

NAVIGATION & MISSION DESIGN BRANCH

SECTION 9 ORBIT DATA - LAUNCH TRAJECTORY

THE ORBITAL MOTION IN LEO REGION: CBERS SATELLITES AND SPACE DEBRIS. Keywords: CBERS Satellites, Space Debris, Orbital Motion, Resonance.

PRELIMINARY DESIGN OF SATELLITE CONSTELLATIONS FOR A BRAZILIAN REGIONAL POSITIONING SYSTEM BY MEANS OF AN EVOLUTIONARY ALGORITHM. Roberto Luiz Galski

PRELIMINARY RESULTS TO SUPPORT EVIDENCE OF THERMOSPHERIC CONTRACTION

Dynamics and Control of Lunisolar Perturbations for. Highly-Eccentric Earth-Orbiting Satellites

CALCULATION OF POSITION AND VELOCITY OF GLONASS SATELLITE BASED ON ANALYTICAL THEORY OF MOTION

Orbital Debris Observation via Laser Illuminated Optical Measurement Techniques

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

List of Tables. Table 3.1 Determination efficiency for circular orbits - Sample problem 1 41

EVALUATING ORBITS WITH POTENTIAL TO USE SOLAR SAIL FOR STATION-KEEPING MANEUVERS

Orbit Representation

Statistical methods to address the compliance of GTO with the French Space Operations Act

EXAMINATION OF THE LIFETIME, EVOLUTION AND RE-ENTRY FEATURES FOR THE "MOLNIYA" TYPE ORBITS

Technical analysis of commercially hosted optical payloads for enhanced SSA

North Korea Satellite Launch

A TLE-BASED REPRESENTATION OF PRECISE ORBIT PREDICTION RESULTS. Jizhang Sang and Bin Li. School of Geodesy and Geomatics, Wuhan University

Short-Arc Correlation and Initial Orbit Determination For Space-Based Observations

EVALUATION OF A SPACECRAFT TRAJECTORY DEVIATION DUE TO THE LUNAR ALBEDO

A SATELLITE MOBILITY MODEL FOR QUALNET NETWORK SIMULATIONS

AUTOMATED FLIGHT DYNAMICS SYSTEM FOR THAICHOTE SATELLITE

Optimization of Orbital Transfer of Electrodynamic Tether Satellite by Nonlinear Programming

Week 02. Assist. Prof. Dr. Himmet KARAMAN

THIRD-BODY PERTURBATION USING A SINGLE AVERAGED MODEL

Comparison of different Methods of Ephemeris Retrieval for Correlation of Observations of Space Debris Objects

APPENDIX B SUMMARY OF ORBITAL MECHANICS RELEVANT TO REMOTE SENSING

COMPARISON OF ANGLES ONLY INITIAL ORBIT DETERMINATION ALGORITHMS FOR SPACE DEBRIS CATALOGUING

Learning Lab Seeing the World through Satellites Eyes

Orbit and Transmit Characteristics of the CloudSat Cloud Profiling Radar (CPR) JPL Document No. D-29695

UPPER ATMOSPHERIC DENSITIES DERIVED FROM STARSHINE SPACECRAFT ORBITS

INVESTIGATING THE SUITABILITY OF ANALYTICAL AND SEMI-ANALYTICAL SATELLITE THEORIES FOR SPACE OBJECT CATALOGUE MAINTENANCE IN GEOSYNCHRONOUS REGIME

Orbit Propagatorr and Geomagnetic Field Estimator for NanoSatellite: The ICUBE Mission

Optimization of Eccentricity during a Two Burn Station Acquisition Sequence of a Geosynchronous Orbit

THE STABILITY OF DISPOSAL ORBITS AT SUPER-SYNCHRONOUS ALTITUDES

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

ATTITUDE CONTROL MECHANIZATION TO DE-ORBIT SATELLITES USING SOLAR SAILS

Design of Orbits and Spacecraft Systems Engineering. Scott Schoneman 13 November 03

ANALYSIS OF THE MEGHA-TROPIQUES TRAJECTORY. DETERMINATION OF RENDEZ-VOUS CONDITIONS WITH THE TERRA SATELLITE.

Lunar Landing Trajectory and Abort Trajectory Integrated Optimization Design.

Study of the Fuel Consumption for Station-Keeping Maneuvers for GEO satellites based on the Integral of the Perturbing Forces over Time

Aerodynamic Lift and Drag Effects on the Orbital Lifetime Low Earth Orbit (LEO) Satellites

Orbits in Geographic Context. Instantaneous Time Solutions Orbit Fixing in Geographic Frame Classical Orbital Elements

Research Article The Impact on Geographic Location Accuracy due to Different Satellite Orbit Ephemerides

AS3010: Introduction to Space Technology

AIR FORCE INSTITUTE OF TECHNOLOGY

SEMI-ANALYTICAL COMPUTATION OF PARTIAL DERIVATIVES AND TRANSITION MATRIX USING STELA SOFTWARE

Third Body Perturbation

Joint Tracking of SMART-1 with VLBI and USB

Chapter 5 - Part 1. Orbit Perturbations. D.Mortari - AERO-423

ANNEX 1. DEFINITION OF ORBITAL PARAMETERS AND IMPORTANT CONCEPTS OF CELESTIAL MECHANICS

CHAPTER 3 PERFORMANCE

GNSS: Global Navigation Satellite Systems

Comparative Study of Basic Constellation Models for Regional Satellite Constellation Design

Transcription:

ARTIFICIAL SATELLITES, Vol. 51, No. 2 2016 DOI: 10.1515/arsa-2016-0005 ACCURACY ASSESSMENT OF GEOSTATIONARY-EARTH-ORBIT WITH SIMPLIFIED PERTURBATIONS MODELS Lihua Ma, Xiaojun Xu, Feng Pang National Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012, China e-mail: mlh@nao.cas.cn ABSTRACT. A two-line element set (TLE) is a data format encoding orbital elements of an Earth-orbiting object for a given epoch. Using suitable prediction formula, the motion state of the object can be obtained at any time. The TLE data representation is specific to the simplified perturbations models, so any algorithm using a TLE as a data source must implement one of these models to correctly compute the state at a specific time. Accurately adjustment of antenna direction on the earth station is the key to satellite communications. With the TLE set topocentric elevation and azimuth direction angles can be calculated. The accuracy of perturbations models directly affect communication signal quality. Therefore, finding the error variations of the satellite orbits is really meaningful. In this present paper, the authors investigate the accuracy of the Geostationary-Earth- Orbit (GEO) with simplified perturbations models. The coordinate residuals of the simplified perturbations models in this paper can give references for engineers to predict the satellite orbits with TLE. Keywords: Geostationary-Earth-Orbit; simplified perturbations models; two-line element set 1. INTRODUCTION A Geostationary-Earth-Orbit (GEO) is a circular orbit 35786 kilometers above Earth s equator and following the direction of Earth s rotation. A satellite in such an orbit has an orbital period equal to Earth s rotational period, and appears motionless at a fixed position in the sky to ground observers. Communications satellites are usually placed in GEO orbit, so that the satellite antennas which communicate with them do not have to real-time rotate to track them, but can be pointed at the position in the sky where the satellites are located. A two-line element set (TLE) is a data format encoding orbital elements of an Earth-orbiting object for a given epoch (Kelso, 1998; Ma et al, 2016). With the simplified perturbations models, orbital state vectors of satellites relative to Earth can be calculated (Vallado et al., 2006; Wei & Zhao, 2009). An earth station plays a vital role in the satellite communications. Accurately adjustment of the antenna angle of direction on the earth station is the key to satellite communications (Roddy, 2006). The direction angle including azimuth and elevation angles can be calculated with the TLE set. The accuracy of perturbations models directly affect communication signal quality. To ensure that the Earth station works reliable the antenna should accurately aim at the target communications satellite. In this present paper, using the Systems Tool Kit (STK) software, the authors investigate the accuracy of the Geostationary- Earth-Orbit (GEO) satellites with simplified perturbations models.

56 2. SIMPLIFIED PERTURBATIONS MODELS Simplified perturbations models are a set of five mathematical models (SGP, SGP4, SDP4, SGP8 and SDP8) (Vallado et al., 2006; Wei & Zhao, 2009). This set of models is often referred to collectively as SGP4 due to the frequency of use of that model particularly with TLE sets produced by the North American Aerospace Defense Command (NORAD) and National Aeronautics and Space Administration (NASA). Based on these models, the effect of perturbations caused by the Earth s shape, drag, radiation, and gravitation effects from other bodies such as the sun and the moon can be predicted. Simplified General Perturbations (SGP) models apply to near Earth objects with an orbital period of less than 225 minutes. Simplified Deep Space Perturbations (SDP) models apply to objects with an orbital period greater than 225 minutes. The original SGP model was developed by Kozai in 1959, refined by Hilton & Kuhlman in 1966 and was originally used by the National Space Surveillance Control Center (and later the United States Space Surveillance Network) for tracking of objects in orbit. SGP8/SDP8 introduced additional improvements for handling orbital decay. Deep space models SDP4 and SDP8 use only simplified drag equations. Accuracy is not a great concern here as high drag satellite cases do not remain in "deep space" for very long as the orbit quickly becomes lower and near circular. SDP4 also adds Lunar-Solar gravity perturbations to all orbits, and Earth resonance terms specifically for 24-hour geostationary and 12-hour Molniya orbits. 3. TLE SET DESCRIPTION As mentioned above, the TLE data representation is specific to the above simplified perturbations models, so any algorithm using a TLE as a data source must implement one of the SGP models to correctly compute the state at a specific time. The TLE sets contain 69- character lines that can be used with NORAD s SGP4/SDP4 orbital model used to determine the position and velocity at a given time. An example TLE for the International Space Station is displayed in Fig. 1. Fig. 1. An example TLE The definitions of fields at first TLE line are given in the following Table. 1. Table 1. TLE first line fields Field Columns Content Example 1 01 01 Line number 1 2 03 07 Satellite number 25544 3 08 08 Classification (U=Unclassified) U 4 10 11 International Designator (Last two digits of launch year) 98 5 12 14 International Designator (Launch number of the year) 067 6 15 17 International Designator (piece of the launch) A 7 19 20 Epoch Year (last two digits of year) 08 8 21 32 Epoch (day of the year and fractional portion of the day) 264.51782528 9 34 43 First Time Derivative of the Mean Motion divided by two.00002182 10 45 52 Second Time Derivative of Mean Motion divided by six (decimal point assumed) 00000-0 11 54 61 BSTAR drag term (decimal point assumed) -11606-4 12 63 63 The number 0 (originally this should have been "Ephemeris type") 0 13 65 68 Element set number. Incremented when a new TLE is generated for this object. 292 14 69 69 Checksum (modulo 10) 7

57 The definitions of fields at second TLE line are given in the following Table. 2. Table 2. TLE second line fields Field Columns Content Example 1 01 01 Line number 2 2 03 07 Satellite number 25544 3 09 16 Inclination (i, degrees) 51.6416 4 18 25 Right ascension of the ascending node (RAAN, degrees) 247.4627 5 27 33 Eccentricity (e, decimal point assumed) 0006703 6 35 42 Argument of perigee (degrees) 130.5360 7 44 51 Mean Anomaly (degrees) 325.0288 8 53 63 Mean Motion (revolutions per day) 15.72125391 9 64 68 Revolution number at epoch (revolutions) 56353 10 69 69 Checksum (modulo 10) 7 4. ACCURACY ANALYSIS 4.1 Simulation software Systems Tool Kit (formerly Satellite Tool Kit) used in this work, is a physics-based software package from Analytical Graphics Inc. It is a suite of software that allows engineers and scientists to design and develop complex dynamic simulations of real-world problems, and allows engineers and scientists to perform complex analyses of ground, sea, air, and space assets, and share results in one integrated solution (Yang, 2005; Ma et al., 2011). The core of STK is a geometry engine for determining the time-dynamic position and attitude of assets, and the spatial relationships among the objects under consideration including their relationships or accesses given a number of complex, simultaneous constraining conditions. Originally created to solve problems involving Earth-orbiting satellites, the software has been used in both the aerospace and defense communities for many other applications. Its common application fields include space exploration, geo-spatial intelligence, spacecraft mission design, missile defense, spacecraft operations, etc. The STK software used in this work was released edition 10.0 in November, 2012. 4.2 Accuracy analysis Actually, orbit elements of a GEO orbit change with time under the spatial perturbation force, thus the GEO satellite does not appear motionless. Refer to present communication satellites CHINASAT-12, ASIASAT-3S and MEASAT-2 with different orbit inclination, the Keplerian orbital elements of three virtual satellites, SAT-1, SAT-2 and SAT-3, are given in this work, respectively. Table 3. Keplerian orbital elements Sat No Epoch year Epoch Semi-major axis (km) e i ( ) RAAN ( ) Argument of periapsis ( ) True anomaly ( ) SAT-1 2015 285.73248328 42164.2801 0.0002867 0.0211 280.870 281.754 169.587 SAT-2 2015 285.87345544 42164.8676 0.0003806 1.2600 81.092 124.896 280.048 SAT-3 2015 285.49450542 42164.2498 0.0009107 6.4969 54.527 155.767 136.603 With the simplified perturbations models the TLE sets of the orbit elements provided in Table 3 are obtained. The information contained in a TLE is a set of mean orbital elements that are specific to the SGP4 propagator, which considers secular and periodic variations due to Earth oblateness, solar and lunar gravitational effects, gravitational resonance effects, and orbital decay using a drag model. Daily coordinate time series are calculated once with the original orbit and also with the TLE sets under the true equator mean equinox (TEME) coordinate system, respectively. Finally, the coordinate residuals of the simplified perturbations models for the three satellites are drawn in the following Figs. 2-4.

58 Fig. 2. Model residuals of SAT-1 Fig. 3. Model residuals of SAT-2 Fig. 4. Model residuals of SAT-3 5. SUMMARY With the STK software, the accuracy of GEO orbits calculated with the simplified perturbations models is investigated. The results show that the model introduces an error of 1.5 kilometers within the whole analysis period. This data is updated frequently in NASA and NORAD sources to limit this error. The coordinate residuals of the simplified perturbations models can give references for engineers to predict the satellite orbits with TLE. Acknowledgements. This work is supported by a grant from the National Natural Science Foundation of China (11573041, 11473045) and the Key Research Program (Grant No. KJCX2-EW-J01). The authors are grateful to CelesTrak (https://celestrak.com) for providing original TLE set and helpful documentation, to the Wikipedia Encyclopedia (https://en.wikipedia.org/wiki/main_page) for helpful documentation.

59 REFERENCES Kelso, T. (1998) Frequently asked questions: two-line element set format. Satellite Times, Vol. 4, No. 3, 52-54 Ma L., Hu C., and Pei J. (2016) A novel polarization tracking method for Earth station antenna. Earth Science Research, Vol. 5, No. 1, 10-19 Ma L., Jing Y., Ji H, and Zhang L. (2011) Analysis of evolution of orbits of GEO satellites near end of life based on the STK software. Astronomical Research & Technology, Vol. 8, No. 4, 347-353 Roddy D. (2006) Satellite Communications (4th Ed.). McGraw-Hill. Vallado D., Crawford P, Hujsak R, and Kelso T. (2006) Revisiting spacetrack report # 3. AIAA, 2006-6753 Wei D, and Zhao C. (2009) Analysis on the accuracy of the SGP4/SDP4 model. Acta Astronomica Sinica, Vol. 50, No. 3, 333-339 Yang Y. (2005) Application of STK in Computer Simulation. Beijing: National Defense Industry Press. Received: 2015-10-28, Reviewed: 2015-12-14, by R. Weber, and 2016-02-29, Accepted: 2016-03-04.