Greetings, All things require introduction and so we begin with ours,

Similar documents
Fundamentals of Satellite technology

Satellite Communications

Keplerian Elements Tutorial

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

Lecture Module 2: Spherical Geometry, Various Axes Systems

Satellite meteorology

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

Experimental Analysis of Low Earth Orbit Satellites due to Atmospheric Perturbations

Astrodynamics (AERO0024)

Creating Satellite Orbits

Astrodynamics (AERO0024)

Orbit Definition. Reference Vector. Vernal (March) Equinox Vector. Sun Vector

MAHALAKSHMI ENGINEERING COLLEGE-TRICHY QUESTION BANK UNIT I PART A

Chapter 2: Orbits and Launching Methods

UNIT 6 CELESTIAL SPHERE AND EQUINOCTIAL SYSTEM OF COORDINATES

How does the solar system, the galaxy, and the universe fit into our understanding of the cosmos?

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

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

On Sun-Synchronous Orbits and Associated Constellations

Astronomy. The Seasons

RECOMMENDATION ITU-R S * Terms and definitions relating to space radiocommunications

The Moon s Orbit. Practical and computational project

Celestial Mechanics and Satellite Orbits

Exercise 1.0 THE CELESTIAL EQUATORIAL COORDINATE SYSTEM

AS3010: Introduction to Space Technology

NAVIGATION & MISSION DESIGN BRANCH

Earth-Centered, Earth-Fixed Coordinate System

What is a Satellite? A satellite is an object that orbits another object. Ex. Radio satellite, moons, planets

Earth Science, 11e. Origin of Modern Astronomy Chapter 21. Early history of astronomy. Early history of astronomy. Early history of astronomy

Ossama Abdelkhalik and Daniele Mortari Department of Aerospace Engineering, Texas A&M University,College Station, TX 77843, USA

orbits Moon, Planets Spacecrafts Calculating the and by Dr. Shiu-Sing TONG

[04] Seasons, Phases, and Eclipses (9/7/17)

Observational Astronomy - Lecture 4 Orbits, Motions, Kepler s and Newton s Laws

Earth Science, 13e Tarbuck & Lutgens

Meridian Circle through Zenith, North Celestial Pole, Zenith Direction Straight Up from Observer. South Celestial Pole

PW-Sat two years on orbit.

The sky and the celestial sphere

lightyears observable universe astronomical unit po- laris perihelion Milky Way

PHYS 160 Astronomy Test #1 Fall 2017 Version B

cosmogony geocentric heliocentric How the Greeks modeled the heavens

If Earth had no tilt, what else would happen?

6/17. Universe from Smallest to Largest:

THE EARTH AND ITS REPRESENTATION

Chapter 1 Review of Equations and Inequalities

AS3010: Introduction to Space Technology

APPENDIX B SUMMARY OF ORBITAL MECHANICS RELEVANT TO REMOTE SENSING

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

Go to Click on the first animation: The north pole, observed from space

A2 Principi di Astrofisica. Coordinate Celesti

Exam #1 Covers material from first day of class, all the way through Tides and Nature of Light Supporting reading chapters 1-5 Some questions are

Astronomy A BEGINNER S GUIDE TO THE UNIVERSE EIGHTH EDITION

Gravitation. Kepler s Law. BSc I SEM II (UNIT I)

The Revolution of the Moons of Jupiter

Astronomy 1143 Quiz 1 Review

[05] Historical Perspectives (9/12/17)

The Celestial Sphere. GEK1506 Heavenly Mathematics: Cultural Astronomy

Celestial Mechanics III. Time and reference frames Orbital elements Calculation of ephemerides Orbit determination

11 Newton s Law of Universal Gravitation

Appearance of the Sky Orientation Motion of sky Seasons Precession (?)

The Reasons for the Seasons. By Allegra Dickson

Understanding Positional Astronomy Part 2 Celestial Co-ordinates Difficulty: Intermediate

3) During retrograde motion a planet appears to be A) dimmer than usual. B) the same brightness as usual C) brighter than usual.

1) Kepler's third law allows us to find the average distance to a planet from observing its period of rotation on its axis.

AST 103 Midterm 1 Review Exam is 3/3/08 in class

Chapter 1: Discovering the Night Sky. The sky is divided into 88 unequal areas that we call constellations.

Astronomy 101 Lab: Lunar Phases and Eclipses

Transforming from Geographic to Celestial Coordinates

2. Modern: A constellation is a region in the sky. Every object in the sky, whether we can see it or not, is part of a constellation.

Fundamentals of Semiconductor Devices Prof. Digbijoy N. Nath Centre for Nano Science and Engineering Indian Institute of Science, Bangalore

Most of the time during full and new phases, the Moon lies above or below the Sun in the sky.

The Sun-Earth-Moon System

The Earth-Moon-Sun System

Physics Lab #6:! Mercury!

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

Appearance of the Sky Orientation Motion of sky Seasons Precession (?)

Modern Physics notes Paul Fendley Lecture 34. Born, chapter III (most of which should be review for you), chapter VII

EE 570: Location and Navigation

Sundials and the Celestial Sphere. Katie Hausknecht

Summary Sheet #1 for Astronomy Main Lesson

Astronomy 100 Section 2 MWF Greg Hall. Outline. Total Lunar Eclipse Time Lapse. Homework #1 is due Friday, 11:50 a.m.!!!!!

Gravitation & Kepler s Laws

The Position of the Sun. Berthold K. P. Horn. necessary to know the position of the sun in the sky. This is particularly

Intensity of Light and Heat. The second reason that scientists prefer the word intensity is Well, see for yourself.

Dynamics of the Earth

CHAPTER 8 PLANETARY MOTIONS

Lecture 15 - Orbit Problems

Chapter 2 Discovering the Universe for Yourself

Geostationary Satellites and Astrophotography

Lunar Motion. V. Lunar Motion. A. The Lunar Calendar. B. Motion of Moon. C. Eclipses. A. The Lunar Calendar. 1) Phases of the Moon. 2) The Lunar Month

Modern Algebra Prof. Manindra Agrawal Department of Computer Science and Engineering Indian Institute of Technology, Kanpur

Gravitation Part I. Ptolemy, Copernicus, Galileo, and Kepler

Spacecraft Dynamics and Control

Astronomy 101: 9/18/2008

Introduction to Global Navigation Satellite System (GNSS) Module: 2

Special Theory of Relativity Prof. Shiva Prasad Department of Physics Indian Institute of Technology, Bombay

THE MOON. G. Iafrate (a), M. Ramella (a) e V. Bologna (b) (a) INAF - Osservatorio Astronomico di Trieste (b)

Seasons Motions of the Sun

Term Project PHYS Solar Rotation

Chapter 2 Discovering the Universe for Yourself

Introduction To Astronomy Lesson 1

Transcription:

-Carina Pereira * & Smit Kamal # *carina.012@hotmail.com #smitkamal@gmail.com Greetings, All things require introduction and so we begin with ours, Most of us are undergraduate college students enrolled in a college located on a small coastal town of south India. We have been working on developing the Attitude Determination and Control Sub-System (ADCS) for our university funded nano-satellite. It s been the most wonderful experience, filled with all the emotions in any spectrum, having learned and gained a great deal we would like to share from our endeavors. The main aim of the blog is to help novices to develop an understanding of the Attitude Determination and Control Sub-System as well as help model one if need be. Explanations pertaining to the same will be as concise and elaborate as possible, we will also explain the system in the required flow with the required amount of detail. Pre-requisite knowledge is kept at a minimum. And so we begin, A nano-satellite, for the unacquainted is just a small satellite of low mass and size (For more information, click on this https://en.wikipedia.org/wiki/miniaturized_satellite). Since the work involved in building a nanosatellite is both widespread and (very) multi-disciplinary, the system has been divided into the following sub-systems (alphabetically listed, or priority wise, depending on your subsystem) (1) Attitude Determination and Control Sub-system This sub-system is primarily responsible for providing (either fine or coarse) pointing accuracy. What this means is being able to point the satellite in a certain direction with a certain degree of accuracy. (2) Communication and Ground Station Sub-system This sub-system is concerned with the transfer of data from the nano-satellite to the ground station and vice versa. (3)Electrical Power Sub-system Since the only source of power in space is solar energy, this sub-system is involved with the harnessing, storing and distribution of power. 1 P a g e

(4) On board data handling Sub-system ADCS FOR BEGINNERS #1 Mostly anything and everything pertaining to the hardware architecture of the on-board computer comes under the umbrella of this sub-system. (5) Payload Payload is the end-goal or the purpose with which the satellite is sent into orbit to begin with. (6) Structures, Thermals and Mechanical Sub-system As the name suggest it is to do with the structure of the satellite, and is responsible for protection of the sub-system both during launch and from the space environment generally. These are the basic sub-systems of our currently in progress nano-satellite, Parikshit (for more information, click on this http://parikshit.org/). Variations to the above system exist considering no nano-satellites are built with exactly the same purpose. Let us begin with the obvious question, Why do we need an ADCS sub-system to begin with? It is both complex to understand and a mouthful to swallow. Well, the ADCS sub-system has been designed to provide both rate and attitude control, this requirement comes from the payload, power and communication sub-systems. The ADCS subsystem can also provide us with the position and velocity of our satellite while in orbit, this is useful for both payload and antenna pointing. As to the question of how is this established? The answer to that question for now is that suitable hardware works in synchronization with complex algorithm. Both aspects should be made clear with the subsequent posts. It Begins With the Frames For a satellite to control its attitude, it needs to know its position along with that of some other stuff wandering in space. This can include a star, sun, moon or other heavenly bodies in our galaxy. Sensors on-board the satellites use these heavenly bodies as a reference to provide vector observations [AAUSAT 3, page 36]. Don t worry if you could not get hold of the last line, things will be clearer as we progress through future lectures. Apart from this, we can also determine the various physical disturbances acting on the satellite in space because of the different heavenly bodies, by accurately knowing their locations. So, the obvious question which hits our curious mind is, how do we make vector observations of things which are zipping around the universe? To record a vector, we need a co-ordinate system, a frame of reference. Now, which frame should we be using to make some larger than life calculations? 2 P a g e

As always, the key to simplify these vector calculations is to take the right frame of reference. And in this situation, where everything, from sun to moon, earth to satellite, is not at all stationary, we need to be extremely careful while selecting the frames and this selection will keep on varying with the observer and the subject. Considering the non-inertial nature of satellites and the heavenly bodies, it will be a respite for us if we observe them from an inertial frame of reference. This stationary nature of observer can help us in easing out our calculations by getting rid of an additional velocity component that could have been imparted from the non-inertial frame. Few of the important things which describe any co-ordinate system are, the fundamental plane(i.e. the X-Y place), the principal direction (i.e. the direction of X axis) and the direction of Z axis. Since the Z-axis must be perpendicular to the fundamental plane. The Y axis is chosen to form the right handed set of coordinate axes. Sounds a bit complicated? Don t mind! You will develop a better idea about these things once we start reading specifically about the different frames. Now, let s talk about our first inertial frame of reference! The Earth Cantered Inertial (ECI) frame! The Earth Cantered Inertial (ECI) frame The Geocentric-Equatorial Coordinate System a.k.a. the Earth Centred Inertial frame has its origin right at the centre of the earth, however it is not fixed to the earth. Although this frame has its origin at the centre of the earth, but it does not rotate with the earth. https://www.youtube.com/watch?v=ue1cfwzxspo, this video can help you better visualize the ECI frame. The red lines in the video denote the three axes of the ECI frame. The fundamental plane contains the equator and the positive X-axis points in the vernal equinox direction. The Z-axis points in the direction of the geographical North Pole and the Y axis consequently completes the right hand set of co-ordinate axes. Here is a picture of this, Any queries? Contact us. We will get back to you. Figure 1. The Earth Centred Inertial(ECI) frame 3 P a g e

Now you might have been wondering, what do we mean by Vernal Equinox? Well, to make things a bit more interesting and to understand other inertial frames we need to throw some light on vernal equinox and something called the Keplerian Elements. Vernal Equinox You might have heard this strange term Vernal Equinox before, and in most cases we have been told that it is "the place in the sky where the sun rises on the first day of Spring". This definition is not just vague and confusing, but it is terrible. Most of us don t have any idea what is the first day of spring and why the sun should be in the same place in the sky on that date every year. To get a better picture of Vernal Equinox, imagine the Sun s orbit around the earth. Yes, right, the earth orbits the sun, but if we start observing from the earth, things will look the other way but the math is equally valid this way too (remember the concept of relative motion?). The plane formed by the hypothetical orbit of the sun around the earth is called the ecliptic. Similar to the ecliptic, we have the equatorial plane, the plane formed by the equator. Now, the sun will intersect the equatorial plane at two points in one orbit, one where the sun crosses the equator while ascending, the point where the sun pops out the equatorial plane and goes up, and the other one when the sun is descending, it punches the equator and dives down before coming up again. If you join these two points, you will get the nodal line for the sun s orbit. Well, well, well, forgot to tell you something, the sun s ascending node is called the Vernal Equinox! Similar to the nodal line of the sun, we have nodal line for the satellites too. These lines are formed by the intersection of the plane formed by satellite s orbit with the equatorial frame. We have made a short video to explain you the ECI frame and the vernal equinox, have a look https://www.youtube.com/watch?v=ge5x5gdjxde Since we have understood the concept of nodal line, let s move forward and understand the Keplerian Elements. Keplerian Elements, also referred as the orbital elements or simply the elements are a set of parameters used to define an elliptical orbit. The first in the list is orbital eccentricity, sometimes referred as eccentricity Eccentricity (e) Eccentricity of an elliptical orbit lies between zero and one. In this domain of zero to one, higher the eccentricity, more elliptical is the orbit. 4 P a g e

Semi major axis (a) Imagine an ellipse traced by the satellite moving around the earth as its focus. The longest possible straight line in this ellipse is its major axis (2a, Figure 2), so half of this is the semi major axis. We made the following video to explain the orbital eccentricity and the semi major axis https://www.youtube.com/watch?v=9mcgdlgdngc Inclination (i) The orbital inclination is the angle between the satellite s orbital plane and the equatorial plane. Orbits having inclination lesser than 90 degrees are called prograde orbit and the orbits with inclination greater than 90 degrees are called retrograde orbit. Satellites in a prograde orbit rotate in the same direction as that of the earth, while those in retrograde, rotate in direction opposite to that of the earth. Next comes the Right Ascension of Ascending node (RAAN) Right Ascension of Ascending node (Ω) Too weird a name, right? Never mind! This is the angle subtended between the nodal line of the sun (vernal equinox side) and that of the satellite (nodal line of the satellite from ascending node side). Well, RAAN is not the only one with a horrible name, one another element with comparatively lesser weird name is the Argument of Perigee We have tried explaining the inclination and the right ascension of ascending node through the following video https://www.youtube.com/watch?v=8dbls9gfrts Argument of Perigee (ω) To visualise this we will have to dig a bit deeper into the satellite s orbit. A satellite in an elliptical orbit will have the earth at one of its focus. So the satellite following the elliptical path around the earth will be closest to the earth at one point of time and farthest at the other. The point where the satellite and our planet maintains the minimum distance is known as perigee, on the other hand, the point where satellite is at the highest possible distance from the earth is called the apogee. 5 P a g e

Figure 2. Elliptical Orbit The vector in the direction from the earth s centre to the perigee defines the eccentricity vector, whose magnitude equals the eccentricity of the orbit. The angle subtended between the eccentricity vector and the nodal line of the satellite marks the Argument of Perigee. True anomaly (θ) Yet another orbital element with another weird name! Consider a vector from earth s origin to the satellite, let s call this vector as the position vector. Now imagine an angle subtended by this vector and the eccentricity vector. This angle is what we call the True anomaly https://www.youtube.com/watch?v=3x6d7xkon90 Mean motion Number of revolution the satellite completes per day. As simple as that! Mean Anomaly For a satellite moving in an elliptical orbit, if we draw a circle which passes through the apogee and perigee of the ellipse and has its centre at the centre of the ellipse, and consider a hypothetical satellite to be moving along that circle with angular velocity equal to the average angular velocity of the satellite moving in the elliptical orbit, then the angle subtended between the position vector of the satellite 6 P a g e

moving on the newly made circle and the eccentricity vector of the elliptical orbit is called the mean anomaly. Still not clear with the mean anomaly? Look at this video https://www.youtube.com/watch?v=y0gnqi2so4w Figure 3. Orbital Elements Now, since we are done with the orbital elements, we can peacefully move on and understand the other reference frames Perifocal Frame This is popularly known as the natural frame for an orbit. This frame is centred at the centre of the earth, the orbital plane is the fundamental plane (XY plane) itself, X axis is directed to the eccentricity vector, Z axis is in the direction of the satellite s angular momentum which lies perpendicular to the orbital plane, and the Y axis completes the right hand set of co-ordinate axis. 7 P a g e

Figure 4. Perifocal Frame Let s now move towards understanding the non-inertial frame. We previously said that an inertial frame helps us in simplifying the calculations, so why are we now bringing the non-inertial frames into picture? One way of answering this question is by looking at the Earth s magnetism. The magnetic field produced by earth differs with the location. So if we have a frame which rotates with the earth, then it will be very convenient to locate different points on earth relative to this moving frame as all points on the earth will be stationary to this frame. This fact is crucial for a satellite having a magnetic field sensor (magnetometer) which needs to know its position with respect to different points of the earth. This non inertial frame is not just important for predicting magnetic field at different points in the orbit but it is also important for any satellite which is bothered about the different points on earth, be it for taking pictures of different parts of the world or for locating the different ground station on the home planet. And last but not the least, the non-inertial frame is the key for analysing the dynamics of a satellite! Earth Centred Earth Fixed (ECEF) Frame This frame keeps on rotating with the Earth. Centred at the equator, it has the equatorial plane as its fundamental plane (XY plane), the X axis can be traced by joining a line starting from the centre of the earth, to the point of intersection of the prime meridian and the equator, the Z axis points towards the geographical north pole and the Y axis completes the right hand set of co-ordinate axes. https://www.youtube.com/watch?v=ue1cfwzxspo The green axes in the video represent the ECEF frame. 8 P a g e

Figure 5. Earth Centred Earth Fixed (ECEF) frame Since the magnetic field produced by the satellite at different points in space in known, the ECEF frame can be used to locate the position of the satellite with respect to the moving earth, and consequently find the magnetic field at that point. The frames we have talked about so far are the ones used to observe the satellite and other things in space from the earth, but then we cannot observe everything from our planet, to stabilise the satellite, we need to change our perspective, we need to look at the things from the satellite. Orbit Reference Frame The orbit reference frame has its origin at the centre of mass of the satellite, the Z axis points towards the centre of mass of the earth, the X axis which is perpendicular to the Z axis, and is in the direction of the velocity of the satellite, and the Y axis completes the right hand set of co-ordinate axis. In this article, the axes of orbit reference frame are denoted with a subscript R (X R, Y R and Z R ). Irrespective of the satellite s orientation in the space, the orbit reference frame will always have its Z axis pointing towards the centre of the Earth, X axis pointing towards the velocity and the Y axis will be completing the right hand set of co-ordinate axes. 9 P a g e

Figure 6. Inertial frame, Orbit Reference Frame and the Satellite Body frame The inertial frame has been denoted by the axes set X I, Y I, and Z I. Satellite Body frame Satellite body frame is fixed to the satellite s body, with its origin at the centre of mass of the satellite. This frame is used to represent the actual satellite in space. The X, Y and Z axis need to be perpendicular to each other and should be popping out of the different faces of the satellite. An example of Satellite Body frame has been given in figure 7. Figure 7. Satellite Body Frame 10 P a g e

NOTES 11 P a g e