Testing the Equivalence principle with LLR
|
|
- Lambert Kennedy
- 6 years ago
- Views:
Transcription
1 Testing the Equivalence principle with LLR F. ignard(*) Observatory of the Côte d Azur, Nice, (France) (*) Thanks to J.. Torre (OCA) for providing the updated LLR documentation F. ignard icroscope ONERA, 30 January
2 Outline Principles of Lunar Laser Ranging Status of the Observations The orbit of the oon The equivalence principle testing Perspective with icroscope F. ignard icroscope ONERA, 30 January
3 LLR in eneral 3 F. ignard icroscope ONERA, 30 January 2013
4 F. ignard icroscope ONERA, 30 January
5 Short story of the LLR Apollo 11: July 1969 first reflectors on the oon surface then Apollo 14, 15, and Lunakhod 1 &2 First returns in the US σ ~ 2 m French attempts at the Pic du idi A. Orzag, O. Calame,.J. Fillol Decision to build a station in rasse (Plateau de Calern) first returns in 1981 Operational station with ruby laser in 1984 σ ~ 20 cm first upgrade to cm station σ ~ 4 cm second upgrade to mm station σ ~ 7 mm fully refurbished station with EO 2004 F. ignard icroscope ONERA, 30 January
6 Why it's difficult Photons sent per laser pulse Way to the oon beam width after atmospheric crossing 4" light on the moon spread over ~ 5 km reflector total area m 2 back to the Earth Corner Cube diffraction 12" light on the moon spread over ~ 20 km collecting area 1 to 10 m 2 Net budget : 1 photon collected every 1 to 10 shots F. ignard icroscope ONERA, 30 January
7 An array of reflectors on the oon (A 14) F. ignard icroscope ONERA, 30 January
8 Location of the reflectors on the oon L1 A15 L2 A14 A11 Not an ideal distribution for selenophysics F. ignard icroscope ONERA, 30 January
9 Observations & Age of the oon Observations as a function of the Lunar phase very important issue for the EP testing the more uniform, the better for the correlation observations at new and full oon have the much weight in the data fitting for EP testing Only 3 observations at the full oon in 1990, 1996 and 2000 during an eclipse F. ignard icroscope ONERA, 30 January
10 Normal points and detected photons Number of returns per normal points at Calern F. ignard icroscope ONERA, 30 January
11 Post fit residuals Evolution de la précision CERA CERA ,1 (2756) 3,8 (2038) 5,1 (1569) Station cdonald cdonald Haleakala ,4 (1622) 4,3 (581) 5,6 (230) 7,9 (455) CERA ,6 (1166) cdonald cdonald ,5 (992) 27,3 (1030) 43 (1487) rms (cm) Chapront et al., 2003 F. ignard icroscope ONERA, 30 January
12 Perturbations on the oon eneral Relativity TL : Earth-oon distance Tidal perturbations Perturbation type Lunar figure Earth's figure Ecliptic plane motion Planetary perturbations (D & ) ain Problem Poissson terms Periodic terms Keplerian motion 1 10^1 10^2 10^3 10^4 10^5 10^6 10^7 10^8 10^9 10^1 Amplitude (cm) 0 Chapront et al., 2003 F. ignard icroscope ONERA, 30 January
13 Where are the LLR stations Not all stations in operation simultaneously today only rasse carries out routine ranges F. ignard icroscope ONERA, 30 January
14 Targets and production Appollo 15 is the most efficient reflector Credit : J. üller et al., F. ignard icroscope ONERA, 30 January
15 Normal Points from different stations 17,000 normal points Credit : J. üller et al., F. ignard icroscope ONERA, 30 January
16 Targets and production 2010 Credit : J. üller et al., F. ignard icroscope ONERA, 30 January
17 Targets and production 2011 Credit : J. üller et al., F. ignard icroscope ONERA, 30 January
18 EO (OCA) Laser Station 18 F. ignard icroscope ONERA, 30 January 2013
19 EO telescope on the Plateau de Calern F. ignard icroscope ONERA, 30 January
20 EO Laser Station Telescope diameter 1.54 m Laser (current hardware) Nd-Yag with frequency doubling Pulse of 200 ps width Energy of 200 mj per pulse credit : J.P artin ~ 1 W!!! Firing rate: 10 Hz Detection APD (Avalanche Photo Diode) in single photon mode Timing for the two-way trip σ < 50 ps ( 1.5 cm) F. ignard icroscope ONERA, 30 January
21 Number of echoes Real restart in 2011 and routine activity in 2012 Appolo X Appolo XV Appolo XV Lunakhod 2 J. Torre et al., 2012 F. ignard icroscope ONERA, 30 January
22 Number of normal points Appolo X Appolo XV Appolo XV Lunakhod 2 J. Torre et al., 2012 F. ignard icroscope ONERA, 30 January
23 EO 2012 : Results number of echoes number of echoes per normal point months months J. Torre et al., 2012 F. ignard icroscope ONERA, 30 January
24 Heliocentric Orbit of the oon 24 F. ignard icroscope ONERA, 30 January 2013
25 Orbit of the oon Look at the oon motion from an heliocentric perspective P moon = days ; a moon = 385,000 km : sampling = 5 days a = 40 4 a moon to enhance the feature F. ignard icroscope ONERA, 30 January
26 Orbit of the oon From an heliocentric perspective P moon = days ; a moon = 385,000 km : sampling = 5 days a = 4a moon change of curvature F. ignard icroscope ONERA, 30 January
27 Orbit of the oon Heliocentric frame a = a moon orbits hardly distinguishable Earth + oon F. ignard icroscope ONERA, 30 January
28 Orbit of the oon Heliocentric frame a = a moon no change of sign of the curvature F. ignard icroscope ONERA, 30 January
29 Provisional conclusion n geocentric frame, the orbit of the oon is a ~ Keplerian motion about the Earth perturbed by the Sun n heliocentric frame, the orbit of the oon is a ~Keplerian motion about the Sun, perturbed by the Earth the oon falls on the Sun more or less as the Earth does The two conclusions seem incompatible, since the forces are identical in both cases? in fact in geocentric frame the action of the Sun is a differential (tidal) effect in 1/r 3 mplications on what is meant by a claimed 'objective' description of a physical reality! several unspoken assumptions F. ignard icroscope ONERA, 30 January
30 Equivalence Principle with LLR 30 F. ignard icroscope ONERA, 30 January 2013
31 Free fall on the oon: Hammer & Feather Painting from true images Apollo 15, David Scott F. ignard icroscope ONERA, 30 January
32 F. ignard icroscope ONERA, 30 January Equations of motion with EP violation Simplified form with Newtonian formulation and Sun-Earth-oon = * SE SE S S SE SE S S E E a E s s μ E E SE SE r E E S S r E i E s E i E s dt d dt d + = = + = = SE SE S S E E a a a E s E i i E E a E a r' E S Heliocentric equations of motions Relative acceleration of oon wrt Earth 3 SE SE a E s δ For the EP term, one has approximately:
33 δa E D λ s S δa s E SE SE 3 γ The EP perturbing force is essentially a constant force directed to/from the Sun quite similar to a radiation pressure nserting in Lagrange planetary equations one gets the observable polarisation on the Earth-oon distance (Nordvedt, 1968) δ r = δ cos D ( m) δ = E With δr to ~ 3cm level, 10 3 to 10 4 observations, one would expect δ to 2x10-14 at the best F. ignard icroscope ONERA, 30 January
34 LLR Data fitting Very complex given the detailed modelling any parameters fitted together station and reflector coordinates, motion and rotation of the oon, nutation, radiation pressure, etc. For the EP testing Primarily done by the JPL team (Williams, Turyshev, Boggs) Latest results with correction for the radiation pressure estimated by Vokrouhlicky (1997) δ = E = 1 ± Williams et al. 2009, Comments: - the uncertainty translates into ~ 4 mm in the cos D amplitude - Accuracy on δ was +/- 2x10-13 in n a presentation to the REX in 2001 said it should be +/- 5x10-14 in 2010!! F. ignard icroscope ONERA, 30 January
35 nterpretation = 1+ SEP + WEP E = 1+η + ω 2 mc WEP : Effect of nuclear composition on the free fall SEP : Coupling of self-energy with gravity E wep = (1 ± 1.4) Adelberger, 2001 then from LLR: E sep = ( 2 ± 2) Williams et al Earth : E g /mc 2 = x oon : E g /mc 2 = x Approx PPN : η = 4β γ 3 η = ± β - 1 ~ ± Williams et al (with γ to 2.3x10-5 ) F. ignard icroscope ONERA, 30 January
36 id-term perspective Very slow improvement with LLR data more observations with EO at OCA no much change regarding new oon and full oon But WEP to be tested to by icroscope LLR will give a better determination of SEP γ to 10-6 with aia from Will, 2007 will lead to better η at the end Also: Bepi Colombo will return β to 3x10-5 independent estimate of η will follow F. ignard icroscope ONERA, 30 January
37 Thanks for your attention F. ignard icroscope ONERA, 30 January
Ranging to Remote Benchmarks
IHP 2006 Experimental Tests of General Relativity John Mester Stanford University Ranging to Remote Benchmarks Lunar Laser Ranging Radar Ranging to Planets Satellite Ranging Shapiro Time Delay Viking Mission
More informationMoon tracking in Grasse MeO station (7845)
Moon tracking in Grasse MeO station (7845) J.M. Torre, G. Martinot-Lagarde, D. Féraudy, M. Aimar, D. Albanese, C. Courde, M. Laas-Bourez, H. Mariey, J. Paris, R. Rigard-Cerison, E. Samain, H Viot MeO LLR
More informationarxiv:gr-qc/ v2 2 Jan 2009
International Journal of Modern Physics D c World Scientific Publishing Company arxiv:gr-qc/0507083v2 2 Jan 2009 LUNAR LASER RANGING TESTS OF THE EQUIVALENCE PRINCIPLE WITH THE EARTH AND MOON JAMES G.
More informationModeling the Earth-Moon Distance for Different Theories of Gravitation
Wellesley College Wellesley College Digital Scholarship and Archive Honors Thesis Collection 2017 Modeling the Earth-Moon Distance for Different Theories of Gravitation Sanaea Rose srose2@wellesley.edu
More informationarxiv:gr-qc/ v1 17 Nov 2006
International Journal of Modern Physics D c World Scientific Publishing Company arxiv:gr-qc/0611095v1 17 Nov 2006 SPACE-BASED TESTS OF GRAVITY WITH LASER RANGING SLAVA G. TURYSHEV, JAMES G. WILLIAMS Jet
More informationShining Dark on Dust. Using Total Lunar Eclipses to expose Dust Accumulation on Apollo Reflectors. Tom Murphy (UCSD)
Shining Dark on Dust Using Total Lunar Eclipses to expose Dust Accumulation on Apollo Reflectors Tom Murphy (UCSD) APOLLO: one giant leap for LLR APOLLO performs lunar laser ranging (LLR) to test the foundations
More informationarxiv:gr-qc/ v1 7 Nov 2003
Improving LLR Tests of Gravitational Theory James G. Williams a, Slava G. Turyshev a, Thomas W. Murphy, Jr. b arxiv:gr-qc/0311021v1 7 Nov 2003 a Jet Propulsion Laboratory, California Institute of Technology,
More informationGaia Astrometry Upkeeping by GNSS - Evaluation Study [GAUGES]
Gaia Astrometry Upkeeping by GNSS - Evaluation Study [GAUGES] M. Gai, A. Vecchiato [INAF-OATo] A. Fienga, F. Vakili, J.P. Rivet, D. Albanese [OCA] Framework: Development of High Precision Astrometric Techniques
More informationAPOLLO: Meeting the Millimeter Goal
APOLLO: Meeting the Millimeter Goal T. W. Murphy, Jr. a, J. D. Strasburg b, C. W. Stubbs c, E. G. Adelberger d, L. Tom c, A. E. Orin a, E. L. Michelsen a, J. Battat c, C. D. Hoyle d, E. Swanson d, E. Williams
More informationPast and Future General Relativity Experiments: Equivalence Principle, Time Delay, and Black Holes. Irwin Shapiro 21 October 2005
Past and Future General Relativity Experiments: Equivalence Principle, Time Delay, and Black Holes Irwin Shapiro 21 October 2005 Translation of Title (a.k.a Outline) Tests of the (Weak) Equivalence Principle
More informationarxiv: v1 [gr-qc] 4 Sep 2012
arxiv:1209.0635v1 [gr-qc] 4 Sep 2012 Planetary ephemerides and gravity tests in the solar system A. Fienga Institut UTINAM, 41 bis avenue de l observatoire Besançon, France We review here the tests of
More informationBasics of Kepler and Newton. Orbits of the planets, moons,
Basics of Kepler and Newton Orbits of the planets, moons, Kepler s Laws, as derived by Newton. Kepler s Laws Universal Law of Gravity Three Laws of Motion Deriving Kepler s Laws Recall: The Copernican
More informationMoonlight project - Observations of Lunar rotation and Ephemeris by optical methods on the Moon
project - Observations of Lunar rotation and Ephemeris by optical methods on the Moon Hideo Hanada 1a, Hiroo Kunimori 2, Mizuhiko Hosokawa 2, Masato Katayama 1b, Hirotomo Noda 1a, Hiroshi Araki 1a, Sho
More informationPerturbations to the Lunar Orbit
Perturbations to the Lunar Orbit th January 006 Abstract In this paper, a general approach to performing perturbation analysis on a two-dimensional orbit is presented. The specific examples of the solar
More informationTesting Genaral Relativity 05/14/2008. Lecture 16 1
There is a big difference between the Newtonian and the Relativistic frameworks: Newtonian: Rigid flat geometry, universal clocks Gravitational force between objects Magic dependence on mass Relativistic:
More informationDevelopment of Software
PPS03-06 Development of Software for Precise LLR Data Analysis and initial results of parameter estimation for lunar motion Ryosuke Nagasawa Sokendai (GUAS) Toshimichi Otsubo Hitotsubashi Univ. Mamoru
More informationLunar Laser Ranging & Tests of General Relativity
Проблемы Современной Астрометрии, Всероссийская конференция-школа для молодых ученых Звенигород, Россия - 22-26 октября 2007 Lunar Laser Ranging & Tests of General Relativity Slava G. Turyshev, James G.
More informationEnd-of-Chapter Exercises
End-of-Chapter Exercises Exercises 1 12 are primarily conceptual questions that are designed to see if you have understood the main concepts of the chapter. Treat all balls with mass as point masses. 1.
More informationGravity with the SKA
Gravity with the SKA Strong-field tests of gravity using Pulsars and Black Holes Michael Kramer Jodrell Bank Observatory University of Manchester With Don Backer, Jim Cordes, Simon Johnston, Joe Lazio
More informationChapter 22 Exam Study Guide
Chapter 22 Exam Study Guide Name: Hour: Date: Multiple Choice Identify the choice that best completes the statement or answers the question. Write the letter that best answers the question or completes
More informationProbing Gravity with 2nd Generation Lunar Laser Ranging
Probing Gravity with 2nd Generation Lunar Laser Ranging Manuele Martini (INFN-LNF) for the MoonLIGHT Collaboration D. G. Currie (PI) University of Maryland at College Park, MD, USA R. Vittori ESA-EAC Astronaut,
More informationEquivalence Principle
July 16, 2015 Universality of free fall (Galileo) Aristoteles view: the manner in which a body falls, does depend on its weight (at least plausible, if one does not abstract from air resistance etc.) Galileo
More informationMonday, October 10, 2011
the shuttle blasts off Then comes the tremendous pressure of three G s and the sudden release into weightlessness as the ship leaves the gravitational field behind -from The Arizona Republic 1 Chapter
More informationTHE LUNAR LIBRATION: COMPARISONS BETWEEN VARIOUS MODELS- A MODEL FITTED TO LLR OBSERVATIONS
THE LUNAR LIBRATION: COMPARISONS BETWEEN VARIOUS MODELS- A MODEL FITTED TO LLR OBSERVATIONS J. CHAPRONT, G. FRANCOU SYRTE - Observatoire de Paris - UMR 8630/CNRS 61, avenue de l Observatoire 75014 Paris
More informationarxiv: v1 [gr-qc] 20 Dec 2007
International Journal of Modern Physics D c World Scientific Publishing Company arxiv:0712.3539v1 [gr-qc] 20 Dec 2007 Laser Ranging for Gravitational, Lunar, and Planetary Science Stephen M. Merkowitz,
More informationVIOLATION OF THE STRONG EQUIVALENCE PRINCIPLE
VIOLATION OF THE STRONG EQUIVALENCE PRINCIPLE KOSTADIN TRENČEVSKI Institute of Mathematics, Ss. Cyril and Methodius University, P. O. Box 1000, Skopje, Macedonia E-mail: kostatre@iunona.pmf.ukim.edu.mk
More informationThe Pioneer Anomaly: Effect, New Data and New Investigation
The Pioneer Anomaly: Effect, New Data and New Investigation Slava G. Turyshev Jet Propulsion Laboratory, California Institute of Technology Seminar at the Sternberg Astronomical Institute Moscow State
More informationLudwig Combrinck HartRAO 3rd Space Geodesy Workshop 16 March 2009 Matjiesfontein
Space Geodesy and Space Science Ludwig Combrinck HartRAO 3rd Space Geodesy Workshop 16 March 2009 Matjiesfontein DST s Concept of Space Science SA Space Agency, commercial applications, CSIR Satellite
More informationarxiv: v2 [physics.ins-det] 1 Nov 2012
Corner-cube retro-reflector instrument for advanced lunar laser ranging Slava G. Turyshev, James G. Williams, William M. Folkner, Gary M. Gutt, Richard T. Baran, Randall C. Hein, Ruwan P. Somawardhana
More information9/13/ Describing Motion: Examples from Everyday Life. Chapter 4: Making Sense of the Universe Understanding Motion, Energy, and Gravity
9/13/17 Lecture Outline 4.1 Describing Motion: Examples from Everyday Life Chapter 4: Making Sense of the Universe Understanding Motion, Energy, and Gravity Our goals for learning: How do we describe motion?
More informationDevelopment of Laser Measurement to Space Debris at Shanghai SLR Station
Abstract Development of Laser Measurement to Space Debris at Shanghai SLR Station Zhang Zhongping, Deng Huarong, Tang Kai, Wu Zhibo, Zhang Haifeng (Shanghai Astronomical Observatory of Chinese Academy
More informationEvaluation of the accuracy of the IAU 2006/2000 precession-nutation
Evaluation of the accuracy of the IAU 2006/2000 precession-nutation Nicole Capitaine (1), Sébastien Lambert (1), Kunliang Yao (1), Jia-cheng Liu (1)(2) (1) SYRTE, Observatoire de Paris, France (2) Nanjing
More informationTests of Lorentz invariance using spinning fermions and laser-ranging ranging to the moon. Eric G. Adelberger University of Washington
Tests of Lorentz invariance using spinning fermions and laser-ranging ranging to the moon Eric G. Adelberger University of Washington cosmic preferred frames? We all were taught that there are no preferred
More informationJean-Pierre Rivet CALERN OBSERVATORY. 26/04/2016 JOVIAL Kick-off Meeting, Nice, April
Jean-Pierre Rivet (jean-pierre.rivet@oca.eu) CALERN OBSERVATORY 26/04/2016 JOVIAL Kick-off Meeting, Nice, April 2016 1 JOVIAL Kick-off Meeting, OCA, April 18th to 21st, 2016 BASIC FACTS Two DSI observing
More information10 General Relativistic Models for Space-time Coordinates and Equations of Motion
10 General Relativistic Models for Space-time Coordinates and Equations of Motion 10.1 Time Coordinates IAU resolution A4 (1991) set the framework presently used to define the barycentric reference system
More information2017 Solar Eclipse. Presentation to Oregon State Legislature Senate Committee on Education. Jim Brau University of Oregon June 6, 2017
2017 Solar Eclipse Presentation to Oregon State Legislature Senate Committee on Education Jim Brau University of Oregon June 6, 2017 Jim Brau, Univ of Oregon June 6, 2017 2017 Solar Eclipse First Total
More informationEVOLUTIONS OF SMALL BODIES IN OUR SOLAR SYSTEM
EVOLUTIONS OF SMALL BODIES IN OUR SOLAR SYSTEM Dynamics and collisional processes Dr. Patrick MICHEL Côte d'azur Observatory Cassiopée Laboratory, CNRS Nice, France 1 Plan Chapter I: A few concepts on
More information7.4 Universal Gravitation
Circular Motion Velocity is a vector quantity, which means that it involves both speed (magnitude) and direction. Therefore an object traveling at a constant speed can still accelerate if the direction
More informationAST 2010 Descriptive Astronomy Study Guide Exam I
AST 2010 Descriptive Astronomy Study Guide Exam I Wayne State University 1 Introduction and overview Identify the most significant structures in the universe: Earth, planets, Sun, solar system, stars,
More informationHow do we describe motion?
Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity 4.1 Describing Motion: Examples from Everyday Life Our goals for learning: How do we describe motion? How is mass different
More informationEstablishment and Observation of Space Debris Laser Ranging
Establishment and Observation of Space Debris Laser Ranging Zhang Zhongping, Zhang Haifeng, Wu Zhibo, Li Pu, Meng Wendong, Chen Juping, Chen WanZhen Shanghai Observatory, Chinese Academy of Sciences Contents:
More informationGeneral Relativity Tests with Pulsars
General Relativity Tests with Pulsars Ingrid Stairs UBC Rencontres de Moriond La Thuile March 25, 2011 Green Bank Telescope Jodrell Bank Parkes Arecibo Outline Intro to pulsar timing Equivalence principle
More informationLRO-LOLA: Measurements of Lunar Altimetry and Surface Conditions
LRO-LOLA: Measurements of Lunar Altimetry and Surface Conditions David E. Smith, MIT Maria T. Zuber, MIT Gregory A. Neumann, GSFC Erwan Mazarico, GSFC and the LOLA Science Team Lunar-Glob Mission International
More informationINTRODUCTION TO ASTRONOMY LAB
INTRODUCTION TO ASTRONOMY LAB Course Design 2002-2003 Course Information Organization: Division: Course Number: PHY 102 Title: Credits: 1 Developed by: Lecture/Lab Ratio: Transfer Status: Extended Registration
More informationThe Properties of Light. Our Window on the Universe
The Properties of Light Chapter 11 Our Window on the Universe Light! And God said, Let there be light: and there was light. And God saw the light, that it was good Genesis 1:3-4 Standing Waves We can create
More informationHYPER 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 informationGENERAL RELATIVITY. The presence of matter affects 4-space.
GENERAL RELATIVITY Whereas Special Relativity is the study of constant velocity motion, General Relativity is associated with situations in which accelerations exist. As gravitation produces acceleration,
More informationGraz in Space Graz SLR System. Daniel Kucharski. IWF / SatGeo
Graz in Space 2008 Graz SLR System Daniel Kucharski IWF / SatGeo Satellite Laser Ranging Range measurements to the satellites - time of flight of the ultrashort laser pulses - mm precision station-satellite
More informationOn the definition and use of the ecliptic in modern astronomy
On the definition and use of the ecliptic in modern astronomy Nicole Capitaine (1), Michael Soffel (2) (1) : Observatoire de Paris / SYRTE (2) : Lohrmann Observatory, Dresden Technical University Introduction
More informationThe Moon as a Test Body for General Relativity
The Moon as a Test Body for General Relativity A White Paper to the Planetary Science Decadal Survey Corresponding Author Stephen M. Merkowitz, NASA Goddard Space Flight Center Stephen.M.Merkowitz@nasa.gov,
More informationIntegration of space and terrestrial techniques to study crustal deformation. Examples in northeastern Italy
Integration of space and terrestrial techniques to study crustal deformation. Examples in northeastern Italy Susanna Zerbini Dipartimento di Fisica, University of Bologna, Italy IAG-IASPEI Joint Capacity
More informationLong-Term Evolution of High Earth Orbits: Effects of Direct Solar Radiation Pressure and Comparison of Trajectory Propagators
Long-Term Evolution of High Earth Orbits: Effects of Direct Solar Radiation Pressure and Comparison of Trajectory Propagators by L. Anselmo and C. Pardini (Luciano.Anselmo@isti.cnr.it & Carmen.Pardini@isti.cnr.it)
More informationTest 1 Review Chapter 1 Our place in the universe
Test 1 Review Bring Gator 1 ID card Bring pencil #2 with eraser No use of calculator or any electronic device during the exam We provide the scantrons Formulas will be projected on the screen You can use
More informationSLR Graz: khz Satellite Laser Ranging & Co
Graz in Space 2014 KFU Graz 4. 5. September 2014 SLR Graz: khz Satellite Laser Ranging & Co Georg Kirchner, Franz Koidl, Oliver Baur Space Research Institute Austrian Academy of Sciences Outline What is
More informationEPM the high-precision planetary ephemerides of IAA RAS for scientific research, astronavigation on the Earth and space
EPM the high-precision planetary ephemerides of IAA RAS for scientific research, astronavigation on the Earth and space Pitjeva E.V. Institute of Applied Astronomy, Russian Academy of Sciences Kutuzov
More informationRadio Science Techniques for Solar System Tests of General Relativity
Radio Science Techniques for Solar System Tests of General Relativity A White Paper submitted to the Fundamental Physical Sciences Panel of the 2009 Decadal Survey on Biological and Physical Sciences in
More informationRecent improvement of the LHD Thomson scattering system
Recent improvement of the LHD Thomson scattering system 1 National Institute for Fusion Science Oroshi 322-6, Toki, Gifu 509-5292, Japan E-mail: yamadai@lhd.nifs.ac.jp H. Funaba, R. Yasuhara, K. Narihara,
More informationLimitations of Newtonian Physics
Limitations of Newtonian Physics 18 th and 19 th Centuries Newtonian Physics was accepted as an ultimate truth Science is never absolute Hundreds of experiments can t prove my theory right but only one
More informationASTR 200 : Lecture 30. More Gravity: Tides, GR, and Gravitational Waves
ASTR 200 : Lecture 30 More Gravity: Tides, GR, and Gravitational Waves 1 Topic One : Tides Differential tidal forces on the Earth. 2 How do tides work???? Think about 3 billiard balls sitting in space
More informationSeminar BELA STAR SIMULATOR
Seminar BELA STAR SIMULATOR Sumita Chakraborty, Michael Affolter, Jakob Neubert (external contractor), Stefan Graf, Daniele Piazza and many more Universität Bern Content > Mercury > BepiColombo > MPO and
More informationTesting General Relativity with Relativistic Binary Pulsars
Testing General Relativity with Relativistic Binary Pulsars Ingrid Stairs UBC GWPAW Milwaukee Jan. 29, 2011 Green Bank Telescope Jodrell Bank Parkes Arecibo Outline Intro to pulsar timing Equivalence principle
More informationChapter 3 The Cycles of the Moon
Chapter 3 The Cycles of the Moon Goals: To understand the phases of the moon To understand how the moon affects tides To understand lunar and solar eclipses To learn some of the history associated with
More information1 General Definitions and Numerical Standards
This chapter provides general definitions for some topics and the values of numerical standards that are used in the document. Those are based on the most recent reports of the appropriate working groups
More informationProton-proton cycle 3 steps PHYS 162 1
Proton-proton cycle 3 steps PHYS 162 1 4 Layers of the Sun CORE : center, where fusion occurs RADIATION: energy transfer by radiation CONVECTION: energy transfer by convection PHOTOSPHERE: what we see
More informationExam# 1 Review Gator 1 Keep the first page of the exam. Scores will be published using the exam number Chapter 0 Charting the Heavens
Exam# 1 Review Exam is Wednesday October 11 h at 10:40AM, room FLG 280 Bring Gator 1 ID card Bring pencil #2 (HB) with eraser. We provide the scantrons No use of calculator or any electronic device during
More informationPhysics 107: Ideas of Modern Physics
Physics 107: Ideas of Modern Physics Exam 2 March 8, 2006 Name ID # Section # On the Scantron sheet, 1) Fill in your name 2) Fill in your student ID # (not your social security #) 3) Fill in your section
More informationTools of Astronomy Tools of Astronomy
Tools of Astronomy Tools of Astronomy The light that comes to Earth from distant objects is the best tool that astronomers can use to learn about the universe. In most cases, there is no other way to study
More informationAST111, 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 informationAnnouncements. HW #2 is online now at MasteringAstronomy.com. Due next Mon at 11pm. For today: finish reading chapter 4.
Announcements HW #2 is online now at MasteringAstronomy.com. Due next Mon at 11pm. For today: finish reading chapter 4. Exam buy-back extra credit due here NOW! Not late extra-credit accepted. Public Service
More information3.4.2 International Laser Ranging Service (ILRS)
3 Reports of IERS components 3.4 Technique Centres 3.4.2 International Laser Ranging Service (ILRS) Introduction Network The International Laser Ranging Service (ILRS), established in 1998, is responsible
More informationAST 103 Midterm 1 Review Exam is 3/3/08 in class
AST 103 Midterm 1 Review Exam is 3/3/08 in class Exam is closed book/closed notes. Formulas will be provided. Bring a No. 2 pencil for the exam and a photo ID. Calculators are OK, but will not be needed.
More informationFundamentals 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 informationStatistics of Photon Arrival Time
Statistics of Photon Arrival Time Tom Murphy February, 001 In an experiment designed to measure the time of arrival of individual photons, it is of critical importance to understand the behavior of the
More informationINPOP new release: INPOP13c
INPOP new release: INPOP13c A. Fienga 1,2, H. Manche 1, J. Laskar 1, M. Gastineau 1, and A. Verma 2 1 Astronomie et Systèmes Dynamiques, IMCCE-CNRS UMR8028, 77 Av. Denfert-Rochereau, 75014 Paris, France
More informationSLR-based orbit determination and orbit prediction of space debris objects
Geodätische Woche Congress Center Essen, 8.- 10. Oktober 2013 SLR-based orbit determination and orbit prediction of space debris objects Harald Wirnsberger, Oliver Baur, Georg Kirchner Space Research Institute
More informationThe Cosmic Perspective Seventh Edition. Making Sense of the Universe: Understanding Motion, Energy, and Gravity. Chapter 4 Lecture
Chapter 4 Lecture The Cosmic Perspective Seventh Edition Making Sense of the Universe: Understanding Motion, Energy, and Gravity 2014 Pearson Education, Inc. Making Sense of the Universe: Understanding
More informationCelestial Mechanics and Orbital Motions. Kepler s Laws Newton s Laws Tidal Forces
Celestial Mechanics and Orbital Motions Kepler s Laws Newton s Laws Tidal Forces Tycho Brahe (1546-1601) Foremost astronomer after the death of Copernicus. King Frederick II of Denmark set him up at Uraniborg,
More informationDetermination of the lunar orbital and rotational parameters and of the ecliptic reference system orientation from LLR measurements and IERS data
Astron. Astrophys. 343, 624 633 (1999) ASTRONOMY AND ASTROPHYSICS Determination of the lunar orbital and rotational parameters and of the ecliptic reference system orientation from LLR measurements and
More informationPHYS 160 Astronomy Test #1 Name Answer Key Test Version A
PHYS 160 Astronomy Test #1 Name Answer Key Test Version A True False Multiple Choice 1. T 1. C 2. F 2. B 3. T 3. A 4. T 4. E 5. T 5. B 6. F 6. A 7. F 7. A 8. T 8. D 9. F 9. D 10. F 10. B 11. B 12. D Definitions
More informationExperimental Tests and Alternative Theories of Gravity
Experimental Tests and Alternative Theories of Gravity Gonzalo J. Olmo Alba gonzalo.olmo@uv.es University of Valencia (Spain) & UW-Milwaukee Experimental Tests and Alternative Theories of Gravity p. 1/2
More informationTests of General Relativity from observations of planets and spacecraft
Tests of General Relativity from observations of planets and spacecraft Pitjeva E.V. Institute of Applied Astronomy, Russian Academy of Sciences Kutuzov Quay 10, St.Petersburg, 191187 Russia e-mail: evp@ipa.nw.ru
More informationIntroduction to General Relativity
Introduction to General Relativity 1 Recall Newtonian gravitation: Clearly not Lorentz invariant, since Laplacian appears rather than d'alembertian. No attempt to find Lorentz invariant equations that
More informationMORE Orbit Determination Software status
MORE Orbit Determination Software status Celestial Mechanics Group University of Pisa Department of Mathematics Progress Meeting MORE, October 15th 2009 1/ 25 Outline 1. Current status of the Orbit14 software
More informationAST101IN Final Exam. 1.) Arrange the objects below from smallest to largest. (3 points)
Name: Possibly useful formulae: AST101IN Final Exam F g = Gm 1 m 2 /r 2 p 2 =a 3 F=ma E=mc 2 1.) Arrange the objects below from smallest to largest. (3 points) The sun The Earth The universe The Milky
More informationPhysics Unit 7: Circular Motion, Universal Gravitation, and Satellite Orbits. Planetary Motion
Physics Unit 7: Circular Motion, Universal Gravitation, and Satellite Orbits Planetary Motion Geocentric Models --Many people prior to the 1500 s viewed the! Earth and the solar system using a! geocentric
More information2. Base your answer to the following question on the diagram below, which has lettered arrows showing the motions of Earth and the Moon.
Practice Moon Test 1. Base your answer to the following question on the information and the cross section below. The cross section represents a possible model of the Moon's interior. Seismographs left
More information4.1 Describing Motion. How do we describe motion? Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity
Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity 4.1 Describing Motion Our goals for learning: How do we describe motion? How is mass different from weight? How do we describe
More informationUseful Formulas and Values
Name Test 1 Planetary and Stellar Astronomy 2017 (Last, First) The exam has 20 multiple choice questions (3 points each) and 8 short answer questions (5 points each). This is a closed-book, closed-notes
More information1) Provide approximate answers for the following questions about the appearance of the Moon.
Astronomy 2110 Fall 2018 Exam 2 October 26, 2018 Part 1: Short qualitative/quantitative questions. Don't over-think these. Answers should be simple and straightforward. If you are spending more than two
More informationChapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity. Copyright 2009 Pearson Education, Inc.
Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity How do we describe motion? Precise definitions to describe motion: Speed: Rate at which object moves speed = distance time
More informationResource Allocation Planning and Scheduling Office. Deep Space Station-15 Out-of-Service Assessment Report. April 11, 2003
Resource Allocation Planning and Scheduling Office Deep Space Station-15 Out-of-Service Assessment Report April 11, 2003 Roger Bartoo Study Description This study describes a Deep Space Network (DSN) loading
More informationChapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity. Copyright 2012 Pearson Education, Inc.
Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity 1 4.1 Describing Motion: Examples from Everyday Life Our goals for learning: How do we describe motion? How is mass different
More informationStars, Galaxies & the Universe (29:50) Professor C.C. Lang Exam #1 - Fall 2010 Wednesday, September 22 nd FORM B - SOLUTIONS
Stars, Galaxies & the Universe (29:50) Professor C.C. Lang Exam #1 - Fall 2010 Wednesday, September 22 nd FORM B - SOLUTIONS Questions 1-6 are True/False questions (worth 4 pts each): 1. The Sun is a Red
More informationGeneral Relativity Tests with Pulsars
General Relativity Tests with Pulsars Ingrid Stairs UBC SLAC Summer Institute July 27, 2005 Much of this material is in Living Reviews in Relativity 2003 5. Pulsars: rotating, magnetized neutron stars.
More informationLecture Outlines. Chapter 5. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.
Lecture Outlines Chapter 5 Astronomy Today 8th Edition Chaisson/McMillan Chapter 5 Telescopes Units of Chapter 5 5.1 Optical Telescopes 5.2 Telescope Size 5.3 Images and Detectors 5.4 High-Resolution Astronomy
More informationHow do we describe motion?
Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity How do we describe motion? Precise definitions to describe motion: Speed: Rate at which object moves $ speed = distance!#"units
More informationCollege Physics B - PHY2054C. Special & General Relativity 11/12/2014. My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building.
Special College - PHY2054C Special & 11/12/2014 My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building Outline Special 1 Special 2 3 4 Special Galilean and Light Galilean and electromagnetism do predict
More informationEffect of Coordinate Switching on Translunar Trajectory Simulation Accuracy
Effect of Coordinate Switching on Translunar Trajectory Simulation Accuracy Mana P. Vautier Auburn University, Auburn, AL, 36849, USA This paper focuses on the affect of round-off error in the accurate
More informationPrinciples of the Global Positioning System Lecture 18" Mathematical models in GPS" Mathematical models used in GPS"
12.540 Principles of the Global Positioning System Lecture 18" Prof. Thomas Herring" Room 54-820A; 253-5941" tah@mit.edu" http://geoweb.mit.edu/~tah/12.540 " Mathematical models in GPS" Review assignment
More informationINTRODUCTION TO ASTRONOMY
Course Information INTRODUCTION TO ASTRONOMY Course Design 2005-2006 Organization EASTERN ARIZONA COLLEGE Division Science & Allied Health Course Number AST 101 Title INTRODUCTION TO ASTRONOMY Credits
More information