ECE 5233 Satellite Communications

Slides:



Advertisements
Similar presentations
ECE 5233 Satellite Communications
Advertisements

MAE 5410 – Astrodynamics Lecture 5 Orbit in Space Coordinate Frames and Time.
GN/MAE155B1 Orbital Mechanics Overview 2 MAE 155B G. Nacouzi.
Space Engineering I – Part I
ARO309 - Astronautics and Spacecraft Design Winter 2014 Try Lam CalPoly Pomona Aerospace Engineering.
Coordinate System & Time/Calendar
Orbital Aspects of Satellite Communications
ECE 5233 Satellite Communications
Introduction to Orbital Mechanics
Prince William Composite Squadron Col M. T. McNeely Presentation for AGI Users Conference CIVIL AIR PATROL PRESENTS The CAP-STK Aerospace Education Program.
ECE 5233 Satellite Communications
ECE 5233 Satellite Communications
Slide 0 SP200, Block III, 1 Dec 05, Orbits and Trajectories UNCLASSIFIED The Two-body Equation of Motion Newton’s Laws gives us: The solution is an orbit.
Prologue Welcome to PH109 Exploring the Universe Dr. Michael L. Cobb Fall, 2003.
What are ground tracks? COE Determination a e i   ? ? ? ? ? ? COE Determination.
Basic Orbital Mechanics Dr. Andrew Ketsdever MAE 5595.
ENGR 215 ~ Dynamics Sections 16.4
Satellite Orbits 인공위성 궤도
Presented by Rehana Jamal (GIS Expert & Geographer) Dated: Advance Applications of RS/GIS in Geo-Environmental Conservation Subject Lecture-6.
The true orbits of visual binaries can be determined from their observed orbits as projected in the plane of the sky. Once the true orbit has been computed,
Chpt. 5: Describing Orbits By: Antonio Batiste. If you’re flying an airplane and the ground controllers call you on the radio to ask where you are and.
Orbital Characteristics of Megha-Tropiques T.Ravindra Babu M.S.Jayashree G.Raju ISRO Satellite Centre Bangalore.
ECE 5233 Satellite Communications
Morehead State University Morehead, KY Prof. Bob Twiggs Understanding Orbits Orbit Facts 1.
Modern Navigation Thomas Herring MW 11:00-12:30 Room
ECE 5233 Satellite Communications
Introduction to Satellite Motion
AT737 Satellite Orbits and Navigation 1. AT737 Satellite Orbits and Navigation2 Newton’s Laws 1.Every body will continue in its state of rest or of uniform.
Announcements: Assignment for Monday: read chapter 4 of text
ECE 5233 Satellite Communications Prepared by: Dr. Ivica Kostanic Lecture 2: Orbital Mechanics (Section 2.1) Spring 2014.
The true orbits of visual binaries can be determined from their observed orbits as projected in the plane of the sky. Once the true orbit has been computed,
The Seasons There would be no seasons if the Earth were not tilted on it’s axis!  Nick Devereux 2006.
CAP-STK Aerospace Program
ECE 5233 Satellite Communications Prepared by: Dr. Ivica Kostanic Lecture 9: Satellite link design (Section 4.3) Spring 2014.
Sept. 25, Apparent motions: Moon, Sun, stars & Orbits Review the daily (diurnal) vs. monthly (sidereal) sky How about the Moon and its phases? Celestial.
University of Colorado Boulder ASEN 5070: Statistical Orbit Determination I Fall 2014 Professor Brandon A. Jones Lecture 3: Basics of Orbit Propagation.
KINEMATICS of a ROLLING BALL Wayne Lawton Department of Mathematics National University of Singapore Lecture based on my student’s MSc.
Phys 214. Planets and Life Dr. Cristina Buzea Department of Physics
Chapter 0 Lecture Charting the Heavens.
A SATELLITE CONSTELLATION TO OBSERVE THE SPECTRAL RADIANCE SHELL OF EARTH Stanley Q. Kidder and Thomas H. Vonder Haar Cooperative Institute for Research.
A Brief Introduction to Astrodynamics
Slide Radian Measure and the Unit Circle. Slide Radian Measure 3.2 Applications of Radian Measure 3.3 The Unit Circle and Circular Functions.
ECE 5233 Satellite Communications
General Motion Rest: Quasars Linear: Stars Keplerian: Binary Perturbed Keplerian: Asteroids, Satellites Complex: Planets, Space Vehicles Rotational: Earth,
Astronomy 105 ä Student Information Sheet ä Class Syllabus ä Lab Syllabus ä Course Supplies ä Text ä Lab Manual ä Scantron 882-ES ä Flashlight with red.
Chapter 5 Satellite orbits Remote Sensing of Ocean Color Instructor: Dr. Cheng-Chien LiuCheng-Chien Liu Department of Earth Science National Cheng-Kung.
Space platform and Orbits Introduction to Remote Sensing Instructor: Dr. Cheng-Chien LiuCheng-Chien Liu Department of Earth Sciences National Cheng Kung.
UNCLASSIFIEDUNCLASSIFIED Lesson 2 Basic Orbital Mechanics A537 SPACE ORIENTATION A537 SPACE ORIENTATION.
University of Colorado Boulder ASEN 5070: Statistical Orbit Determination I Fall 2015 Professor Brandon A. Jones Lecture 3: Time and Coordinate Systems.
ASEN 5050 SPACEFLIGHT DYNAMICS Two-Body Motion Prof. Jeffrey S. Parker University of Colorado – Boulder Lecture 3: The Two Body Problem 1.
Sea Launch/Zenit Thrust: 8,180,000 N Fueled Weight: 450,000 kg Payload to LEO: 13,740 kg Cost per launch: $100,000,000 Cost per kg: $7,300 Launches: 31/28.
AS 3004 Stellar Dynamics Energy of Orbit Energy of orbit is E = T+W; (KE + PE) –where V is the speed in the relative orbit Hence the total Energy is is.
ECE 5233 Satellite Communications Prepared by: Dr. Ivica Kostanic Lecture 19: Multiple Access Schemes (4) (Section 6.8) Spring 2011.
INTRODUCTION TO DYNAMICS ANALYSIS OF ROBOTS (Part 4)
Transformation, Translation, Reflection, and Rotation Kristin Gibson.
ASTR Spring 2008 Joel E. Tohline, Alumni Professor 247 Nicholson Hall [Slides from Lecture04]
Categories of Satellites
University of Colorado Boulder ASEN 5070: Statistical Orbit Determination I Fall 2015 Professor Brandon A. Jones Lecture 2: Basics of Orbit Propagation.
INTRODUCTION TO DYNAMICS ANALYSIS OF ROBOTS (Part 1)
INTRODUCTION TO DYNAMICS ANALYSIS OF ROBOTS (Part 2)
Learning from the Past, Looking to the Future James R. (Jim) Beaty, PhD - NASA Langley Research Center Vehicle Analysis Branch, Systems Analysis & Concepts.
AE Review Orbital Mechanics.
Space Mechanics.
Astronomy 340 Fall 2005 Class #3 13 September 2005.
به نام خدا تعیین مدار.
Orbit in Space Coordinate Frames and Time
Rotational Kinematics
Next we will use global information about the Earth to help define and understand how the A-Train orbits the Earth.
MODULE 1.
A e i o u.
Presentation transcript:

ECE 5233 Satellite Communications Prepared by: Dr. Ivica Kostanic Lecture 3: Orbital Elements (Sections 2.2-2.7) Spring 2014

Outline Orbital elements (geocentric equatorial coordinates) Rotating coordinate system Two Line Element (TLE) data Mapping between coordinate systems Examples Important note: Slides present summary of the results. Detailed derivations are given in notes.

Geocentric equatorial coordinate system (GEC) GEC – fixed rectangular coordinate system GEC – moves through the space, but does not rotate Used in astronomy to map the sky The angles of interest W - right ascension – angle from positive x-axis to the point where satellite comes out of the equatorial plane i – inclination of the orbit – angle between orbital plane and equatorial plane w – argument of perigee – angular distance between perigee and the point where the satellite comes out of the equatorial plane X axis points to “first point of Aries” – distant star All satellites have their GEC coordinates given in “Two line elements” (TLE) data

Example: Two line data for space station TLE data – used by NORAD and NASA TLA – data is used for precise calculations of satellite positions Access: http://celestrak.com/NORAD/elements/

Rotating rectangular system Natural way to view space objects if you are on Earth System is fixed to the Earth (i.e. it translates and rotates along with the Earth) X-axis goes through (0,0) lat-lon point In summary: 3 systems are used Orbital systems GEC system Rotating system Position of the satellite is mapped between the coordinated systems using linear transformations Angular velocity of Earths rotation (72 urad/sec) Time since last alignment between GEC and rotating system Rotating and GEC systems align once/day (at different times)

Transformation between coordinate systems Mapping between orbital system and GEC Mapping between GEC and rotating system Mapping between orbital and and rotating system

Calculation of t – time in min after Universal Time midnight Angle between GEC and rotating system t – time in min after Universal Time midnight Julian day reference point: Noon of December 31st, 1899; Start of JD 2415020 JD calculator: http://www.nr.com/julian.html

Example: calculate WeTe for January 15th, 2011 at 5PM EST Calculation of Example: calculate WeTe for January 15th, 2011 at 5PM EST 1. Calculate t (A:1320) 2. Determine JD (A: 2455577) 3. Use spreadsheet above Answer: ~ 85 degrees

Six orbital elements To specify position of a satellite one needs 6 orbital elements Selection somewhat arbitrary Quantities adopted by the text Eccentricity (e) Semi-major axis (a) Time at the perigee (tp) Right ascending node angle (W) Inclination (i) Argument of the perigee (w) Quantities adopted by the TLE data Eccentricity (e) Mean motion in rev/day (Mm) Mean anomaly (M) Right ascending node angle (W) Inclination (i) Argument of the perigee (w) Note: TLE data is given for a given time reference For calculation of time at perigee For calculation of semi-major axis

Example 1. Calculate rotating coordinates for ISS at the time when TLE data are taken TLE Data for ISS (obtained on OCT 26, 2013): 1 25544U 98067A 13298.22562148 .00015844 00000-0 27472 -3 0 8812 2 25544 51.6491 184.0276 0002282 77.2230 68.9667 15.4953682854871 Note: Calculation details are given in notes. Some results are as follows: Eccentric anomaly E = 1.204173 Semi-major axis: a = 6783.8km Orbital coordinates: x0 = 2430.21km; y0 = 6332.95km Rotating coordinates: xr = -4201.9km, yr = -4428.57km, zr = 2957.01km