Thermal Radiation Effects on Deep-Space Satellites Part 2

Size: px
Start display at page:

Download "Thermal Radiation Effects on Deep-Space Satellites Part 2"

Transcription

1 Thermal Radiation Effects on Deep-Space Satellites Part 2 Jozef C. Van der Ha Fundamental Physics in Space, Bremen October 27, 2017

2 Table of Contents Mercury Properties & Parameters Messenger Satellite Model Overview of SRP & TRP Models SRP & TRP Analytical Results Mercury Temperature Model Geometry & Orbital Models Results for Infra-Red & Albedo Effects Conclusion JvdHa-2

3 Mercury Orbital & Thermal Characteristics Mercury s Orbit has High Eccentricity and Inclination: e M 0.2; i M 7 Mercury has High Daytime Surface Temperatures (2 nd after Venus!): up to 720 K = 450 C but only 100 K at Night Mercury s Rotation Rate is 1.5 Times its Mean Orbital Rate (i.e., 3 : 2 Resonance between Rotation and Orbit Motion) Mercury s Day (i.e., Time between two Sun Passages over the Same Meridian) is Extremely Long: 176 Earth Days As a Result, Variations in Local Solar Elevation and Surface Thermal Characteristics Occur only very Gradually Mercury s Rotation Axis is Close ( 0.01 ) to Orbit Plane Normal Subsolar Points are Practically on Equator At Perihelia (Aphelia) They are Called: Hot (Warm) Poles JvdHa-3

4 Variation of Solar Radiation Energy e 0.2 JvdHa-4

5 Mercury s Orbital & Thermal Input Parameters a : Mercury s orbital semi-major axis in [AU] e : Mercury s orbital eccentricity i : Mercury s orbital inclination 7.00 Ω : Mercury s longitude of ascending node ω : Mercury s longitude of perihelion M : Mercury s mean longitude µ M : Mercury s gravitational parameter (GM) in [km 3 s -2 ] R M : Mercury s equatorial (and polar) radius in [km] o M : Mercury s obliquity of rotation axis to orbit plane 0 P rot : Mercury s sidereal rotational period in [days] P orb : Mercury s sidereal orbital period in [days] P syn : Mercury s synodic orbital period in [days] d M : Mercurian day in [days] A b : Mercury s Bond albedo coefficient 0.12 α M : Mercury s surface thermal absorption coefficient 0.88 ε M : Mercury s surface thermal emissivity coefficient 0.82 JvdHa-5

6 Mercury s Unique Thermal Environment Mercury s Incident Solar Flux is much Higher than Earth s Non-Gravitational Effects on Satellite Solar Radiation (SR) Satellite s Thermal Radiation (TR) Mercury s Infra-Red Radiation (IR) Mercury s Albedo Reflection (AL) JvdHa-6

7 Messenger Unique Trajectory Design End of Life: April 2015 JvdHa-7

8 Messenger Orbiting Mercury JvdHa-8

9 Messenger In-Flight Spacecraft Configuration JvdHa-9

10 SRP Input Parameters for 10-Plates Configuration ID Component Area RA DE ρ s ρ d 1 X- Sunshield wing Center Sunshield X+ Sunshield wing X facing (2-way) Z facing (2-way) Y+ facing (backside) X+ Solar panel, front X- Solar panel, front X+ Solar panel, back X- Solar panel, back JvdHa-10

11 Accelerations due to Solar Radiation Pressure Total Acceleration Induced by SRP on Satellite with n Surfaces A j a = a + a + a SRP, j absorbed, j specular, j diffuse, j n {( ) ( ) }, a = c A cosϑ 1 ρ s+ 2 ρ / 3 + ρ cosϑ n SRP SRP j j s j d s j j j = 1 n { } 2 a = c A f s+ g n [m / s ] SRP SRP j j j j j = 1 JvdHa-11

12 Accelerations due to Thermal Heat Flux Recoil Acceleration due to Thermal Radiation Diffuse Emission I 0 n θ I = I 0 cosθ Emitted Heat Flux: 2 a = C Ther Ther n m s 3 with: qther = εσt 2 [ / ] 4 Flat Surface (Temperature T) a Ther C Ther Factor 2/3 is due to Lambert s Law 4 qther A εσt A = = c m c m 2 [ m/ s ] A: Area m: Satellite Mass c: Speed of Light JvdHa-12

13 SRP Inputs & Acceleration Results (at Perihelion) For Ideal Attitude, Symmetry Assures that SRP Force is Along y-axis Parameters Arrays Sunshields # 1, 2, 3 area (m 2 ): projected area (m 2 ): C-SRP (m/s 2 ): E E E E-07 α : ρ : ρ s : ρ d : mass (kg): 700 Accelerations (m/s 2 ): E E E E-07 Total Acceleration (m/s 2 ): E-07 JvdHa-13

14 SRP Induced Acceleration Results over Orbit JvdHa-14

15 TRP Inputs & Acceleration Results (at Perihelion) Ideal Attitude Assures that also TRP-Induced Force is Along y-axis Parameters Arrays Sunshields # 1, 2, 3 area (m 2 ): C-TRP(m/s 2 ): 1.472E E E E-19 alpha: epsilon: mass (kg): 700 Accelerations (m/s 2 ): E E E E-08 Percentages (%): Total Acceleration (m/s 2 ): E-07 (= 15.2 % of SRP) JvdHa-15

16 TRP Induced Acceleration Results over Orbit JvdHa-16

17 Variation of Temperature over Orbit - 1 Too High! Operating Temperatures of Solar Cells Should be < 150 C JvdHa-17

18 Variation of Temperatures over Orbit - 2 Therefore, Solar Arrays Must be Off-Pointed by Angle of 25 Operating Temperature Limit for Solar Cells JvdHa-18

19 Mercury Sub-Solar Latitudinal Temperature Model Heat Balance Conditions for Infinitesimal Latitude Bands T S ( d ) = M αm S σεmd 2 M 0.25 (, ) = ( )( cos ) T d ϕ T d ϕ 0.25 P M S M TS o = 723 K ( Perihelium) JvdHa-19

20 Mercury Surface Temperature as Function of Phi Angle JvdHa-20

21 Mercury Hemispherical Temperature Model Heat Balance Condition over Entire Daylight Hemisphere α S ( πr ) ( )( 2 ) M = σεm TM dm πrm M dm αm S TM ( dm ) = 2 2 σεmdm 0.25 This Hemispherical Temperature is (0.5) 0.25 = 84.1 % of Subsolar T S When Using Baseline Values α M = 0.88 and ε M = 0.82, We Find Equilibrium Temperatures over Mercury s Daylight Hemisphere: 608 K at Mercury s perihelion 494 K at Mercury s aphelion JvdHa-21

22 Geometry of Mercury Albedo Reflection on Satellite JvdHa-22

23 Grid Configuration over Mercury s Surface AZ i = π + 2π az i 1 EL j = π 2 + π el ( ) ( for i =1,2,...,az) ( j 0.5) ( for j =1,2,...,el) Number of grids: Azimuth : az = 100 Elevation : el = 50 Grid point position vector: R ij = R M cos EL j cos AZ i cos EL j sin AZ i = R M n ij sin EL j n ij : unit surface normal at g ij JvdHa-23

24 Geometrical View-Factor Modeling for IR & AL View Factor: f cosδ cosδ 1, ij 2, ij, k ij, k = 2 π rij A k If δ 1,ij π/2 or δ 2,ij,k π/2: f ij,k = 0 JvdHa-24

25 Modular Simulink Model for Mercury Orbiter JvdHa-25

26 SIMULINK SPACECRAFT MODEL JvdHa-26

27 Messenger Orbit about Mercury Mercury-Sun Coordinate System P M, Q M, W M MESSENGER ORBIT: a = km Period = 12 h e = 0.74 i = ω = JvdHa-27

28 Visualization of Messenger Test Orbits Noon-Midnight Orbit Dawn-Dusk Orbit JvdHa-28

29 Analytical & Numerical Results JvdHa-29

30 Accelerations over Mercury Year (Simulink) Red: SR Green: TR Blue: IR Yellow: AL JvdHa-30

31 Conclusions Solar Radiation Intensity at Mercury is up to 10 x Larger than at Earth Location We Present Analyses & Results of SR, TR, IR, & AL Radiation Effects on the Mercury Orbiter MESSENGER by Means of Analytical & Numerical Approaches TR & IR Effects Introduce Appreciable Accelerations on Messenger Trajectory with Both up to 25 % of SRP AL Effect is Appreciable only over a Small Interval and is Significantly Smaller than TR & IR : 5 % of SRP High-Fidelity Thermal Models are Essential for Robust Satellite Thermal Subsystem Design Also they Improve Deep-Space Navigation by Enhancing Trajectory Prediction Models JvdHa-31

32 Our Publications on Thermal Radiation - 1 JvdHa-32

33 Our Publications on Thermal Radiation - 2 JvdHa-33

Lecture 19: The Moon & Mercury. The Moon & Mercury. The Moon & Mercury

Lecture 19: The Moon & Mercury. The Moon & Mercury. The Moon & Mercury Lecture 19: The Moon & Mercury The Moon & Mercury The Moon and Mercury are similar in some ways They both have: Heavily cratered Dark colored surfaces No atmosphere No water They also have some interesting

More information

Calculation of the Gravitational Constant. Abstract. + α R 2 1. T 3 cos 12 β

Calculation of the Gravitational Constant. Abstract. + α R 2 1. T 3 cos 12 β Calculation of the Gravitational Constant Abstract G 4 M ( π 5 α 2 ω + α R 2 tan θ R 2 2 ω 20T 5 cos 20 β π 3 α 2 ω 8 ω 2G4 T 3 cos 2 β G is the Gravitational constant and M is the mass of Earth. ω Angular

More information

Fundamentals of Satellite technology

Fundamentals of Satellite technology Fundamentals of Satellite technology Prepared by A.Kaviyarasu Assistant Professor Department of Aerospace Engineering Madras Institute Of Technology Chromepet, Chennai Orbital Plane All of the planets,

More information

Appendix C. Mercury Retro-Reflection Modelling and Effects on MPO Solar Array. Anja Frey Giulio Tonellotto (ESA/ESTEC, The Netherlands)

Appendix C. Mercury Retro-Reflection Modelling and Effects on MPO Solar Array. Anja Frey Giulio Tonellotto (ESA/ESTEC, The Netherlands) 51 Appendix C Mercury Retro-Reflection Modelling and Effects on MPO Solar Array Anja Frey Giulio Tonellotto (ESA/ESTEC, The Netherlands) 9 th European Space Thermal Analysis Workshop 3 November 15 5 Mercury

More information

Thermal Design of the Solar Array in a Low Earth Orbit Satellite by Analytical and Numerical Methods

Thermal Design of the Solar Array in a Low Earth Orbit Satellite by Analytical and Numerical Methods Thermal Design of the Solar Array in a Low Earth Orbit Satellite by Analytical and Numerical Methods Korea Aerospace Research Institute Hui-Kyung Kim*, Jang-Joon Lee, Bum-Seok Hyun and Cho-Young Han Background

More information

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

Orbit Definition. Reference Vector. Vernal (March) Equinox Vector. Sun Vector Simulation: TMG Thermal Analysis User's Guide Orbit Definition TMG can model three types of orbits: Beta Angle, Geostationary and Classical. For Earth, three special classical orbits are already partially

More information

Astronomy 111 Exam Review Problems (Real exam will be Tuesday Oct 25, 2016)

Astronomy 111 Exam Review Problems (Real exam will be Tuesday Oct 25, 2016) Astronomy 111 Exam Review Problems (Real exam will be Tuesday Oct 25, 2016) Actual Exam rules: you may consult only one page of formulas and constants and a calculator while taking this test. You may not

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

is a revolution relative to a fixed celestial position. is the instant of transit of mean equinox relative to a fixed meridian position.

is a revolution relative to a fixed celestial position. is the instant of transit of mean equinox relative to a fixed meridian position. PERIODICITY FORMULAS: Sidereal Orbit Tropical Year Eclipse Year Anomalistic Year Sidereal Lunar Orbit Lunar Mean Daily Sidereal Motion Lunar Synodical Period Centenial General Precession Longitude (365.25636042

More information

Lecture #03. January 20, 2010, Wednesday

Lecture #03. January 20, 2010, Wednesday Lecture #03 January 20, 2010, Wednesday Causes of Earth s Seasons Earth-Sun geometry Day length Solar angle (beam spread) Atmospheric beam depletion Shape and Size of the Earth North Pole E Geoid: not

More information

Radiation from planets

Radiation from planets Chapter 4 Radiation from planets We consider first basic, mostly photometric radiation parameters for solar system planets which can be easily compared with existing or future observations of extra-solar

More information

In all cases assume the observer is located at the latitude of Charlottesville (38 degrees north).

In all cases assume the observer is located at the latitude of Charlottesville (38 degrees north). 1. Recalling that azimuth is measured around the sky from North (North is 0 degrees, East is 90 degrees, South is 180 degrees, and West is 270 degrees) estimate (do not calculate precisely) the azimuth

More information

Astrodynamics (AERO0024)

Astrodynamics (AERO0024) Astrodynamics (AERO0024) 5. Dominant Perturbations Gaëtan Kerschen Space Structures & Systems Lab (S3L) Motivation Assumption of a two-body system in which the central body acts gravitationally as a point

More information

Astronomy 111 Review Problems Solutions

Astronomy 111 Review Problems Solutions Astronomy 111 Review Problems Solutions Problem 1: Venus has an equatorial radius of 6052 km. Its semi-major axis is 0.72 AU. The Sun has a radius of cm. a) During a Venus transit (such as occurred June

More information

Lecture 2c: Satellite Orbits

Lecture 2c: Satellite Orbits Lecture 2c: Satellite Orbits Outline 1. Newton s Laws of Mo3on 2. Newton s Law of Universal Gravita3on 3. Kepler s Laws 4. Pu>ng Newton and Kepler s Laws together and applying them to the Earth-satellite

More information

Feasible Mission Designs for Solar Probe Plus to Launch in 2015, 2016, 2017, or November 19, 2008

Feasible Mission Designs for Solar Probe Plus to Launch in 2015, 2016, 2017, or November 19, 2008 Feasible Mission Designs for Solar Probe Plus to Launch in 2015, 2016, 2017, or 2018 2007 Solar Probe Study & Mission Requirements Trajectory study and mission design trades were conducted in the fall

More information

1. SOLAR GEOMETRY, EXTRATERRESTRIAL IRRADIANCE & INCIDENCE ANGLES

1. SOLAR GEOMETRY, EXTRATERRESTRIAL IRRADIANCE & INCIDENCE ANGLES 1. SOLAR GEOMETRY, EXTRATERRESTRIAL IRRADIANCE & INCIDENCE ANGLES The Sun A blackbody with T ~ 6000 K Blackbody radiation with the same amount of energy per unit of area T ~ 5762 K Blackbody radiating

More information

Astrodynamics (AERO0024)

Astrodynamics (AERO0024) Astrodynamics (AERO0024) 5. Dominant Perturbations Gaëtan Kerschen Space Structures & Systems Lab (S3L) Motivation Assumption of a two-body system in which the central body acts gravitationally as a point

More information

Third Body Perturbation

Third Body Perturbation Third Body Perturbation p. 1/30 Third Body Perturbation Modeling the Space Environment Manuel Ruiz Delgado European Masters in Aeronautics and Space E.T.S.I. Aeronáuticos Universidad Politécnica de Madrid

More information

Satellite Communications

Satellite Communications Satellite Communications Lecture (3) Chapter 2.1 1 Gravitational Force Newton s 2nd Law: r r F = m a Newton s Law Of Universal Gravitation (assuming point masses or spheres): Putting these together: r

More information

Lecture 3: Global Energy Cycle

Lecture 3: Global Energy Cycle Lecture 3: Global Energy Cycle Planetary energy balance Greenhouse Effect Vertical energy balance Latitudinal energy balance Seasonal and diurnal cycles Solar Flux and Flux Density Solar Luminosity (L)

More information

Energy. Kinetic and Potential Energy. Kinetic Energy. Kinetic energy the energy of motion

Energy. Kinetic and Potential Energy. Kinetic Energy. Kinetic energy the energy of motion Introduction to Climatology GEOGRAPHY 300 Tom Giambelluca University of Hawai i at Mānoa Solar Radiation and the Seasons Energy Energy: The ability to do work Energy: Force applied over a distance kg m

More information

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

MAE 180A: Spacecraft Guidance I, Summer 2009 Homework 2 Due Tuesday, July 14, in class. MAE 180A: Spacecraft Guidance I, Summer 2009 Homework 2 Due Tuesday, July 14, in class. Guidelines: Please turn in a neat and clean homework that gives all the formulae that you have used as well as details

More information

AT622 Section 5 The Sun

AT622 Section 5 The Sun AT622 Section 5 The Sun The main aim here is to acquaint the student with basic radiative properties of the sun and the factors that govern the disposition of solar radiation received at Earth. 5.1 The

More information

Geometry of Earth Sun System

Geometry of Earth Sun System 12S56 Geometry of Earth Sun System Figure below shows the basic geometry Northern Hemisphere Winter ω equator Earth s Orbit Ecliptic ω ω SUN equator Northern Hemisphere Spring Northern Hemisphere Fall

More information

AST111 PROBLEM SET 6 SOLUTIONS

AST111 PROBLEM SET 6 SOLUTIONS AST111 PROBLEM SET 6 SOLUTIONS Homework problems 1. Ideal gases in pressure balance Consider a parcel of molecular hydrogen at a temperature of 100 K in proximity to a parcel of ionized hydrogen at a temperature

More information

ATMS 321 Problem Set 1 30 March 2012 due Friday 6 April. 1. Using the radii of Earth and Sun, calculate the ratio of Sun s volume to Earth s volume.

ATMS 321 Problem Set 1 30 March 2012 due Friday 6 April. 1. Using the radii of Earth and Sun, calculate the ratio of Sun s volume to Earth s volume. ATMS 321 Problem Set 1 30 March 2012 due Friday 6 April 1. Using the radii of Earth and Sun, calculate the ratio of Sun s volume to Earth s volume. 2. The Earth-Sun distance varies from its mean by ±1.75%

More information

ME 476 Solar Energy UNIT THREE SOLAR RADIATION

ME 476 Solar Energy UNIT THREE SOLAR RADIATION ME 476 Solar Energy UNIT THREE SOLAR RADIATION Unit Outline 2 What is the sun? Radiation from the sun Factors affecting solar radiation Atmospheric effects Solar radiation intensity Air mass Seasonal variations

More information

SOLUTIONS. F 0 λ1 T = (1) F 0 λ2 T = (2) ε = (6) F 0 λt = (7) F 0 λt = (11)

SOLUTIONS. F 0 λ1 T = (1) F 0 λ2 T = (2) ε = (6) F 0 λt = (7) F 0 λt = (11) Federal University of Rio Grande do Sul Mechanical Engineering Department MEC0065 - Thermal Radiation Professor - Francis Name: Márleson Rôndiner dos Santos Ferreira SOLUTIONS Question 2-5: The total hemispherical

More information

Solar Insolation and Earth Radiation Budget Measurements

Solar Insolation and Earth Radiation Budget Measurements Week 13: November 19-23 Solar Insolation and Earth Radiation Budget Measurements Topics: 1. Daily solar insolation calculations 2. Orbital variations effect on insolation 3. Total solar irradiance measurements

More information

(b) The period T and the angular frequency ω of uniform rotation are related to the cyclic frequency f as. , ω = 2πf =

(b) The period T and the angular frequency ω of uniform rotation are related to the cyclic frequency f as. , ω = 2πf = PHY 302 K. Solutions for problem set #9. Non-textbook problem #1: (a) Rotation frequency of 1 Hz means one revolution per second, or 60 revolutions per minute (RPM). The pre-lp vinyl disks rotated at 78

More information

Modern Navigation. Thomas Herring

Modern Navigation. Thomas Herring 12.215 Modern Navigation Thomas Herring Review of Monday s Class Spherical Trigonometry Review plane trigonometry Concepts in Spherical Trigonometry Distance measures Azimuths and bearings Basic formulas:

More information

Observer-Sun Angles. ), Solar altitude angle (α s. ) and solar azimuth angle (γ s )). θ z. = 90 o α s

Observer-Sun Angles. ), Solar altitude angle (α s. ) and solar azimuth angle (γ s )). θ z. = 90 o α s Observer-Sun Angles Direction of Beam Radiation: The geometric relationships between a plane of any particular orientation relative to the earth at any time and the incoming beam solar radiation can be

More information

HYPER Industrial Feasibility Study Final Presentation Orbit Selection

HYPER Industrial Feasibility Study Final Presentation Orbit Selection Industrial Feasibility Study Final Presentation Orbit Selection Steve Kemble Astrium Ltd. 6 March 2003 Mission Analysis Lense Thiring effect and orbit requirements Orbital environment Gravity Atmospheric

More information

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

Orbits in Geographic Context. Instantaneous Time Solutions Orbit Fixing in Geographic Frame Classical Orbital Elements Orbits in Geographic Context Instantaneous Time Solutions Orbit Fixing in Geographic Frame Classical Orbital Elements Instantaneous Time Solutions Solution of central force motion, described through two

More information

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

Observational Astronomy - Lecture 4 Orbits, Motions, Kepler s and Newton s Laws Observational Astronomy - Lecture 4 Orbits, Motions, Kepler s and Newton s Laws Craig Lage New York University - Department of Physics craig.lage@nyu.edu February 24, 2014 1 / 21 Tycho Brahe s Equatorial

More information

Earth s Motions. Rotation -!! Period of Rotation - amount of time to make one complete rotation Example: Earth rotates in hours.

Earth s Motions. Rotation -!! Period of Rotation - amount of time to make one complete rotation Example: Earth rotates in hours. Name: Date: Period: Earth In the Solar System The Physical Setting: Earth Science CLASS NOTES! Rotation -! Period of Rotation - amount of time to make one complete rotation Example: Earth rotates in hours

More information

E d. h, c o, k are all parameters from quantum physics. We need not worry about their precise definition here.

E d. h, c o, k are all parameters from quantum physics. We need not worry about their precise definition here. The actual form of Plank s law is: b db d b 5 e C C2 1 T 1 where: C 1 = 2hc o 2 = 3.7210 8 Wm /m 2 C 2 = hc o /k = 1.3910 mk Where: h, c o, k are all parameters from quantum physics. We need not worry

More information

EVALUATION OF A SPACECRAFT TRAJECTORY DEVIATION DUE TO THE LUNAR ALBEDO

EVALUATION OF A SPACECRAFT TRAJECTORY DEVIATION DUE TO THE LUNAR ALBEDO ISSN 76-58 nd International Congress of Mechanical Engineering (COBEM 3) November 3-7, 3, Ribeirão Preto, SP, Brazil Copyright 3 by ABCM EVALUATION OF A SPACECRAFT TRAJECTORY DEVIATION DUE TO THE LUNAR

More information

USAAAO First Round 2015

USAAAO First Round 2015 USAAAO First Round 2015 This round consists of 30 multiple-choice problems to be completed in 75 minutes. You may only use a scientific calculator and a table of constants during the test. The top 50%

More information

Data and formulas at the end. Exam would be Weds. May 8, 2008

Data and formulas at the end. Exam would be Weds. May 8, 2008 ATMS 321: Science of Climate Practice Mid Term Exam - Spring 2008 page 1 Atmospheric Sciences 321 Science of Climate Practice Mid-Term Examination: Would be Closed Book Data and formulas at the end. Exam

More information

Radiation in climate models.

Radiation in climate models. Lecture. Radiation in climate models. Objectives:. A hierarchy of the climate models.. Radiative and radiative-convective equilibrium.. Examples of simple energy balance models.. Radiation in the atmospheric

More information

Astronomy 111 Practice Final Exam

Astronomy 111 Practice Final Exam Astronomy 111 Practice Final Exam Prof. Douglass Fall 2018 Name: If this were a real exam, you would be reminded of the Exam rules here: You may consult only one page of formulas and constants and a calculator

More information

APPENDIX B SUMMARY OF ORBITAL MECHANICS RELEVANT TO REMOTE SENSING

APPENDIX B SUMMARY OF ORBITAL MECHANICS RELEVANT TO REMOTE SENSING APPENDIX B SUMMARY OF ORBITAL MECHANICS RELEVANT TO REMOTE SENSING Orbit selection and sensor characteristics are closely related to the strategy required to achieve the desired results. Different types

More information

Chapter Seven. Solar Energy

Chapter Seven. Solar Energy Chapter Seven Solar Energy Why Studying Solar energy To know the heat gain or heat loss in a building In making energy studies In the design of solar passive homes. Thermal Radiation Solar spectrum is

More information

HEATING THE ATMOSPHERE

HEATING THE ATMOSPHERE HEATING THE ATMOSPHERE Earth and Sun 99.9% of Earth s heat comes from Sun But

More information

Design optimization of a Solar Panel Angle and its Application to CubeSat 'CADRE'

Design optimization of a Solar Panel Angle and its Application to CubeSat 'CADRE' 1th Annual Cubesat Developer s Workshop Design optimization of a Solar Panel Angle and its Application to CubeSat 'CADRE' Dae Young Lee, James W. Cutler Introduction Many CubeSats are power constrained.

More information

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

ANNEX 1. DEFINITION OF ORBITAL PARAMETERS AND IMPORTANT CONCEPTS OF CELESTIAL MECHANICS ANNEX 1. DEFINITION OF ORBITAL PARAMETERS AND IMPORTANT CONCEPTS OF CELESTIAL MECHANICS A1.1. Kepler s laws Johannes Kepler (1571-1630) discovered the laws of orbital motion, now called Kepler's laws.

More information

A study upon Eris. I. Describing and characterizing the orbit of Eris around the Sun. I. Breda 1

A study upon Eris. I. Describing and characterizing the orbit of Eris around the Sun. I. Breda 1 Astronomy & Astrophysics manuscript no. Eris c ESO 2013 March 27, 2013 A study upon Eris I. Describing and characterizing the orbit of Eris around the Sun I. Breda 1 Faculty of Sciences (FCUP), University

More information

AS3010: Introduction to Space Technology

AS3010: Introduction to Space Technology AS3010: Introduction to Space Technology L E C T U R E S 8-9 Part B, Lectures 8-9 23 March, 2017 C O N T E N T S In this lecture, we will look at factors that cause an orbit to change over time orbital

More information

Jupiter: Giant of the Solar System

Jupiter: Giant of the Solar System Jupiter: Giant of the Solar System Jupiter s Red spot : A huge storm that has raged for over 300 years that is ~2x size of the Earth. Gas Giant is really a Liquid Giant! Pictures over ~7 years from Hubble

More information

The Earth is a Rotating Sphere

The Earth is a Rotating Sphere The Earth is a Rotating Sphere The Shape of the Earth Earth s Rotation ( and relative movement of the Sun and Moon) The Geographic Grid Map Projections Global Time The Earth s Revolution around the Sun

More information

Name and Student ID Section Day/Time:

Name and Student ID Section Day/Time: AY2 - Overview of the Universe - Midterm #1 - Instructor: Maria F. Duran Name and Student ID Section Day/Time: 1) Imagine we ve discovered a planet orbiting another star at 1 AU every 6 months. The planet

More information

Earth s Orbit. Sun Earth Relationships Ridha Hamidi, Ph.D. ESCI-61 Introduction to Photovoltaic Technology

Earth s Orbit. Sun Earth Relationships Ridha Hamidi, Ph.D. ESCI-61 Introduction to Photovoltaic Technology 1 ESCI-61 Introduction to Photovoltaic Technology Sun Earth Relationships Ridha Hamidi, Ph.D. Spring (sun aims directly at equator) Winter (northern hemisphere 23.5 tilts away from sun) 2 Solar radiation

More information

S CIENCE O VERVIEW. 59 Lesson Plan. Standards Benchmarks. Science Overview. Lesson Overview. Answer Key. Resources. My Angle on Cooling ME S S EN G ER

S CIENCE O VERVIEW. 59 Lesson Plan. Standards Benchmarks. Science Overview. Lesson Overview. Answer Key. Resources. My Angle on Cooling ME S S EN G ER S CIENCE O VERVIEW There are many different ways to cope with being in the presence of a hot object. A familiar one is to move away from it so that you do not feel its heat as strongly. Another is to change

More information

Fundamentals of Astrodynamics and Applications

Fundamentals of Astrodynamics and Applications Fundamentals of Astrodynamics and Applications Third Edition David A. Vallado with technical contributions by Wayne D. McClain Space Technology Library Published Jointly by Microcosm Press Hawthorne, CA

More information

Chapter 1 Solar Radiation

Chapter 1 Solar Radiation Chapter 1 Solar Radiation THE SUN The sun is a sphere of intensely hot gaseous matter with a diameter of 1.39 10 9 m It is, on the average, 1.5 10 11 m away from the earth. The sun rotates on its axis

More information

Chapter 2. Heating Earth's Surface & Atmosphere

Chapter 2. Heating Earth's Surface & Atmosphere Chapter 2 Heating Earth's Surface & Atmosphere Topics Earth-Sun Relationships Energy, Heat and Temperature Mechanisms of Heat Transfer What happens to Incoming Solar Radiation? Radiation Emitted by the

More information

Lecture 3. Background materials. Planetary radiative equilibrium TOA outgoing radiation = TOA incoming radiation Figure 3.1

Lecture 3. Background materials. Planetary radiative equilibrium TOA outgoing radiation = TOA incoming radiation Figure 3.1 Lecture 3. Changes in planetary albedo. Is there a clear signal caused by aerosols and clouds? Outline: 1. Background materials. 2. Papers for class discussion: Palle et al., Changes in Earth s reflectance

More information

Lecture 11: Meridonal structure of the atmosphere

Lecture 11: Meridonal structure of the atmosphere Lecture 11: Meridonal structure of the atmosphere September 28, 2003 1 Meridional structure of the atmosphere In previous lectures we have focussed on the vertical structure of the atmosphere. Today, we

More information

Heriot-Watt University

Heriot-Watt University Heriot-Watt University Distinctly Global www.hw.ac.uk Thermodynamics By Peter Cumber Prerequisites Interest in thermodynamics Some ability in calculus (multiple integrals) Good understanding of conduction

More information

Earth s orbit. 2.2 Celestial mechanics. Earth s orbit. Earth s orbit. Variation of eccentricity over Earth s history. 0 e 1

Earth s orbit. 2.2 Celestial mechanics. Earth s orbit. Earth s orbit. Variation of eccentricity over Earth s history. 0 e 1 around the un:. Celestial mechanics Earth's orbit is an ellipse and the sun is located in one of its focal points. Definition Ellipse: The sum of the distances from any point on the ellipse to the two

More information

Sunlight and its Properties II. EE 446/646 Y. Baghzouz

Sunlight and its Properties II. EE 446/646 Y. Baghzouz Sunlight and its Properties II EE 446/646 Y. Baghzouz Solar Time (ST) and Civil (clock) Time (CT) There are two adjustments that need to be made in order to convert ST to CT: The first is the Longitude

More information

The current climate epoch: The Holocene

The current climate epoch: The Holocene Lecture 1: Climate and the 1st Law of Thermodynamics Quick Review of Monday s main features: Lapse rate, Hydrostatic Balance surface = 288K (15 C). In lowest 10 km, the lapse rate, Γ, averages: T Γ

More information

Sunlight and its Properties Part I. EE 446/646 Y. Baghzouz

Sunlight and its Properties Part I. EE 446/646 Y. Baghzouz Sunlight and its Properties Part I EE 446/646 Y. Baghzouz The Sun a Thermonuclear Furnace The sun is a hot sphere of gas whose internal temperatures reach over 20 million deg. K. Nuclear fusion reaction

More information

Appendix E. Development of a thermal control system for South Africa s next generation Earth observation satellite

Appendix E. Development of a thermal control system for South Africa s next generation Earth observation satellite 51 Appendix E Development of a thermal control system for South Africa s next generation Earth observation satellite Daniël van der Merwe (DENEL Spaceteq, South Africa) 52 Development of a thermal control

More information

Physics 3/3/2013. Kepler s Three Laws of Planetary Motion. Distance, Velocity from the Sun at any given time: q=angle from perihelion

Physics 3/3/2013. Kepler s Three Laws of Planetary Motion. Distance, Velocity from the Sun at any given time: q=angle from perihelion Physics Kepler s Three Laws of Planetary Motion a=semi-major axis b=semi-minor axis e=eccentricity Focus, Foci Distance, Velocity from the Sun at any given time: a(1 e ) r 1 ecosq v 1 GM ro a q=angle from

More information

Satellite meteorology

Satellite meteorology GPHS 422 Satellite meteorology GPHS 422 Satellite meteorology Lecture 1 6 July 2012 Course outline 2012 2 Course outline 2012 - continued 10:00 to 12:00 3 Course outline 2012 - continued 4 Some reading

More information

Callisto's Rotation Equations Peyman Parsa November 15, Updated July 2012

Callisto's Rotation Equations Peyman Parsa November 15, Updated July 2012 Callisto's Rotation Equations Peyman Parsa November 5, 004 - Updated July 0 www.peymanparsa.com Constants f R 79.86 i M 0.7036 i St.06470 i Ma 5.69647970 0 i Sp.06868490 9 Free Rotation Constant Maximum

More information

The Sun. Fabio Peron Università IUAV - Venezia. Earth-Sun relationships. The Sun. Photosphere (Emits much of the solar radiant power)

The Sun. Fabio Peron Università IUAV - Venezia. Earth-Sun relationships. The Sun. Photosphere (Emits much of the solar radiant power) Università IUAV Venezia Corso di Fisica Tecnica Ambientale Laboratorio Integrato Innovazione-Sostenibilità Sun and solar radiation Fabio Peron Università IUAV - Venezia The Sun The Sun Earth-Sun relationships

More information

Data and formulas at the end. Real exam is Wednesday May 8, 2002

Data and formulas at the end. Real exam is Wednesday May 8, 2002 ATMS 31: Physical Climatology Practice Mid Term Exam - Spring 001 page 1 Atmospheric Sciences 31 Physical Climatology Practice Mid-Term Examination: Would be Closed Book Data and formulas at the end. Real

More information

Seasonal & Diurnal Temp Variations. Earth-Sun Distance. Eccentricity 2/2/2010. ATS351 Lecture 3

Seasonal & Diurnal Temp Variations. Earth-Sun Distance. Eccentricity 2/2/2010. ATS351 Lecture 3 Seasonal & Diurnal Temp Variations ATS351 Lecture 3 Earth-Sun Distance Change in distance has only a minimal effect on seasonal temperature. Note that during the N. hemisphere winter, we are CLOSER to

More information

PROBLEM cos 30. With A 1 = A 2 = A 3 = A 4 = 10-3 m 2 and the incident radiation rates q 1-j from the results of Example 12.

PROBLEM cos 30. With A 1 = A 2 = A 3 = A 4 = 10-3 m 2 and the incident radiation rates q 1-j from the results of Example 12. PROBLEM. KNON: Rate at which radiation is intercepted by each of three surfaces (see (Example.). FIND: Irradiation, G[/m ], at each of the three surfaces. ANALYSIS: The irradiation at a surface is the

More information

v lim a t = d v dt a n = v2 R curvature

v lim a t = d v dt a n = v2 R curvature PHY 02 K. Solutions for Problem set # 6. Textbook problem 5.27: The acceleration vector a of the particle has two components, the tangential acceleration a t d v dt v lim t 0 t (1) parallel to the velocity

More information

Thermal Systems Design MARYLAND. Fundamentals of heat transfer Radiative equilibrium Surface properties Non-ideal effects

Thermal Systems Design MARYLAND. Fundamentals of heat transfer Radiative equilibrium Surface properties Non-ideal effects Thermal Systems Design Fundamentals of heat transfer Radiative equilibrium Surface properties Non-ideal effects Internal power generation Environmental temperatures Conduction Thermal system components

More information

Orbit Representation

Orbit Representation 7.1 Fundamentals 223 For this purpose, code-pseudorange and carrier observations are made of all visible satellites at all monitor stations. The data are corrected for ionospheric and tropospheric delays,

More information

2. Illustration of Atmospheric Greenhouse Effect with Simple Models

2. Illustration of Atmospheric Greenhouse Effect with Simple Models 2. Illustration of Atmospheric Greenhouse Effect with Simple Models In the first lecture, I introduced the concept of global energy balance and talked about the greenhouse effect. Today we will address

More information

Defunct Satellites, Rotation Rates and the YORP Effect. Antonella A. Albuja and Daniel J. Scheeres University of Colorado - Boulder, Boulder, CO, USA

Defunct Satellites, Rotation Rates and the YORP Effect. Antonella A. Albuja and Daniel J. Scheeres University of Colorado - Boulder, Boulder, CO, USA Defunct Satellites, Rotation Rates and the YORP Effect Antonella A. Albuja and Daniel J. Scheeres University of Colorado - Boulder, Boulder, CO, USA ABSTRACT With the amount of space debris found in Earth

More information

Chapter S1 Lecture. The Cosmic Perspective Seventh Edition. Celestial Timekeeping and Navigation Pearson Education, Inc.

Chapter S1 Lecture. The Cosmic Perspective Seventh Edition. Celestial Timekeeping and Navigation Pearson Education, Inc. Chapter S1 Lecture The Cosmic Perspective Seventh Edition Celestial Timekeeping and Navigation 2014 Pearson Education, Inc. Celestial Timekeeping and Navigation 2014 Pearson Education, Inc. S1.1 Astronomical

More information

Problem A: Solar Sailing to Mars

Problem A: Solar Sailing to Mars Problem A: Solar Sailing to Mars Team 670 November 13, 017 Abstract Solar sails became reality lately, being far more affordable then most of modern methods of propulsion in space. They obviously have

More information

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

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 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 concept questions, some involve working with equations,

More information

UNIT 6 CELESTIAL SPHERE AND EQUINOCTIAL SYSTEM OF COORDINATES

UNIT 6 CELESTIAL SPHERE AND EQUINOCTIAL SYSTEM OF COORDINATES UNIT 6 CELESTIAL SPHERE AND EQUINOCTIAL SYSTEM OF COORDINATES Structure 6.1 Introduction Objectives 6.2 References 6.3 Apparent Annual Motion of the Sun and the Concept of the Ecliptic and the Obliquity

More information

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

Chapter 1: Discovering the Night Sky. The sky is divided into 88 unequal areas that we call constellations. Chapter 1: Discovering the Night Sky Constellations: Recognizable patterns of the brighter stars that have been derived from ancient legends. Different cultures have associated the patterns with their

More information

CHAPTER 8 PLANETARY MOTIONS

CHAPTER 8 PLANETARY MOTIONS 1 CHAPTER 8 PLANETARY MOTIONS 8.1 Introduction The word planet means wanderer (πλάνητες αστέρες wandering stars); in contrast to the fixed stars, the planets wander around on the celestial sphere, sometimes

More information

1.2 Energy sources and fluxes on planets. (Recommended reading: Ingersoll (2013), p ; Pierrehumbert (2010), Chap. 3).

1.2 Energy sources and fluxes on planets. (Recommended reading: Ingersoll (2013), p ; Pierrehumbert (2010), Chap. 3). 1.2 Energy sources and fluxes on planets. (Recommended reading: Ingersoll (2013), p. 33-53; Pierrehumbert (2010), Chap. 3). 1.2.1 Planetary Energy Sources Sources of free energy are fundamental for climate

More information

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

Sail-Assisted End-of-Life Disposal of High-LEO Satellites 4th International Symposium on Solar Sailing Kyoto, Japan, January 17-20, 2017 Sail-Assisted End-of-Life Disposal of High-LEO Satellites Sergey Trofimov Keldysh Institute of Applied Mathematics Russian

More information

Thermal Systems Design

Thermal Systems Design Thermal Systems Design Fundamentals of heat transfer Radiative equilibrium Surface properties Non-ideal effects Internal power generation Environmental temperatures Conduction Thermal system components

More information

Radiation in the atmosphere

Radiation in the atmosphere Radiation in the atmosphere Flux and intensity Blackbody radiation in a nutshell Solar constant Interaction of radiation with matter Absorption of solar radiation Scattering Radiative transfer Irradiance

More information

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

Celestial Mechanics III. Time and reference frames Orbital elements Calculation of ephemerides Orbit determination Celestial Mechanics III Time and reference frames Orbital elements Calculation of ephemerides Orbit determination Orbital position versus time: The choice of units Gravitational constant: SI units ([m],[kg],[s])

More information

Dynamical properties of the Solar System. Second Kepler s Law. Dynamics of planetary orbits. ν: true anomaly

Dynamical properties of the Solar System. Second Kepler s Law. Dynamics of planetary orbits. ν: true anomaly First Kepler s Law The secondary body moves in an elliptical orbit, with the primary body at the focus Valid for bound orbits with E < 0 The conservation of the total energy E yields a constant semi-major

More information

r p L = = So Jupiter has the greater angular momentum.

r p L = = So Jupiter has the greater angular momentum. USAAAO 2015 Second Round Solutions Problem 1 T 10000 K, m 5, d 150 pc m M 5 log(d/10) M m 5 log(d/10) 5 5 log(15) 0.88 We compare this with the absolute magnitude of the sun, 4.83. solar 100 (4.83 0.88)/5

More information

SPACECRAFT FORMATION CONTROL IN VICINITY OF LIBRATION POINTS USING SOLAR SAILS

SPACECRAFT FORMATION CONTROL IN VICINITY OF LIBRATION POINTS USING SOLAR SAILS SPACECRAFT FORMATION CONTROL IN VICINITY OF LIBRATION POINTS USING SOLAR SAILS D. Novikov (1), R. Nazirov (), N. Eismont (3) (1) E-mail: dnovikov@iki.rssi.ru () E-mail: rnazirov@rssi.ru (3) E-mail: neismont@iki.rssi.ru

More information

CLASSICS. Handbook of Solar Radiation Data for India

CLASSICS. Handbook of Solar Radiation Data for India Solar radiation data is necessary for calculating cooling load for buildings, prediction of local air temperature and for the estimating power that can be generated from photovoltaic cells. Solar radiation

More information

Response to Unified Theory of Climate

Response to Unified Theory of Climate Response to Unified Theory of Climate Dr. Daniel M. Sweger National College Introduction During the last two years that I have been teaching Environmental Science and attempting to explain global warming

More information

NAVIGATION & MISSION DESIGN BRANCH

NAVIGATION & MISSION DESIGN BRANCH c o d e 5 9 5 National Aeronautics and Space Administration Michael Mesarch Michael.A.Mesarch@nasa.gov NAVIGATION & MISSION DESIGN BRANCH www.nasa.gov Outline Orbital Elements Orbital Precession Differential

More information

Unit 2: Celestial Mechanics

Unit 2: Celestial Mechanics Unit 2: Celestial Mechanics The position of the Earth Ptolemy (90 168 AD) Made tables that allowed a user to locate the position of a planet at any past, present, or future date. In order to maintain circular

More information

Chapter S1 Celestial Timekeeping and Navigation. How do we define the day, month, year, and planetary time periods?

Chapter S1 Celestial Timekeeping and Navigation. How do we define the day, month, year, and planetary time periods? Chapter S1 Celestial Timekeeping and Navigation S1.1 Astronomical Time Periods Our goals for learning:! How do we define the day, month, year, and planetary time periods?! How do we tell the time of day?!

More information

Satellite Orbital Maneuvers and Transfers. Dr Ugur GUVEN

Satellite Orbital Maneuvers and Transfers. Dr Ugur GUVEN Satellite Orbital Maneuvers and Transfers Dr Ugur GUVEN Orbit Maneuvers At some point during the lifetime of most space vehicles or satellites, we must change one or more of the orbital elements. For example,

More information

Calculating equation coefficients

Calculating equation coefficients Solar Energy 1 Calculating equation coefficients Construction Conservation Equation Surface Conservation Equation Fluid Conservation Equation needs flow estimation needs radiation and convection estimation

More information

arxiv: v1 [physics.pop-ph] 29 May 2009

arxiv: v1 [physics.pop-ph] 29 May 2009 Gravity assist in 3D like in Ulysses mission Herbert Morales Escuela de Física, Universidad de Costa Rica, San José, Costa Rica arxiv:0905.4788v1 [physics.pop-ph] 29 May 2009 (Dated: October 22, 2018)

More information