Initial Highlights from the Gould Belt Survey
|
|
|
- Jonah Mason
- 9 years ago
- Views:
Transcription
1 Initial Highlights from the Gould Belt Survey Philippe André, CEA/SAp Saclay A.Men shchikov, S.Bontemps, V. Könyves, F. Motte, N. Schneider, P. Didelon, V. Minier, P. Saraceno, D.Ward- Thompson, J. Di Francesco, G. White, S. Molinari, L. Testi, A. Abergel, M. Griffin, T. Henning, P. Royer, B. Merin, R. Vavrek, M. Attard, D. Arzoumanian, C.D. Wilson, P. Martin, and the Gould Belt KP Consortium Main groups : SPIRE SAG 3 (eg. J.Kirk, M. Huang, G. Olofsson) CEA Saclay, IFSI Rome & INAF Arcetri PACS PACS PACS Institutes OAMP Marseille (A. Zavagno) KU Leuven (J. Blommaert & C. Waelkens) MPIA Heidelberg (O. Krause, R. Launhardt) + ESA HSC ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
2 The Herschel Gould Belt Survey SPIRE/PACS µm imaging of the bulk of nearby (d < 0.5 kpc) molecular clouds (~ 160 deg 2 ), mostly located in Gould s Belt. Gould Belt Cepheus Serpens Ophiuchus Lupus Taurus Perseus Aquila Chamaeleon CrA Orion IRAS 100 µm Motivation: Key issues on the early stages of star formation What determines the distribution of stellar masses = the IMF? What generates prestellar cores and what governs their evolution to protostars and proto-brown dwarfs? Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
3 First images from the Gould Belt Survey 1) Polaris translucent cloud (d ~ 150 pc) 23 Oct 2009 Red : SPIRE 500 µm Green : SPIRE 250 µm Blue : PACS 160 µm ~ 7 deg 2 field Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010 Ward-Thompson et al Miville-Deschênes et al A&A special issue
4 First images from the Gould Belt Survey 2) Aquila Rift star-forming cloud (d ~ 260 pc) 24 Oct 2009 cf. Red : SPIRE 500 µm Green : SPIRE 160 µm Blue : PACS 70 µm ~ 3.3 deg x 3.3 deg field Könyves et al Bontemps et al André et al A&A special issue
5 Revealing the structure of one of the nearest infrared dark clouds (Aquila Main: d ~ 260 pc) Herschel (SPIRE+PACS) Dust temperature map (K) Herschel (SPIRE+PACS) Column density map (H 2 /cm 2 ) W40 1 deg ~ 4.5 pc Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May
6 Aquila: `Compact Source Extraction (using getsources A. Menshchikov et al. 2010) Herschel (SPIRE+PACS) Aquila entire field: N H2 (cm -2 ) Spatial distribution of extracted cores 541 starless 201 YSOs Starless = neither PACS 70 µ nor Spitzer 24 µ emission % of the cores found at N H2 > 7x10 21 cm -2 A v (back) > 7 3 deg ~ 14 pc 70/160/500 µm composite image
7 Aquila: `Compact Source Extraction (using getsources A. Menshchikov et al. 2010) Herschel (SPIRE+PACS) Aquila entire field: N H2 (cm -2 ) Spatial distribution of extracted cores 541 starless 201 YSOs Starless = neither PACS 70 µ nor Spitzer 24 µ emission 80% of the cores found at A v (back) > 7 3 deg ~ 14 pc 70/160/500 µm composite image
8 Aquila/Serpens-South dark filament: A rich protocluster in the making Spitzer/IRAC 8 µm SPIRE 250 µm + PACS 160/70 µ m 10 ~ 0.75 pc Gutermuth et al. 2008: 54 Class I YSOs Bontemps et al. 2010: 8 Class 0 protostars
9 A group of starless cores in Aquila-East Herschel (SPIRE+PACS) N H2 map (cm -2 ) Radial intensity profiles Ellipses: FWHM sizes of 24 starless cores at 250 µm Stars ( ) : Two candidate Class 0 protostars Könyves et al. 2010, A&A special issue Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010 Background subtracted
10 Most of the Aquila starless cores are bound Motte et al. (2001) Mass, M (M ) Cirrus noise limit in Aquila Likely prestellar in nature Könyves et al Talk by V. Könyves on Thursday Deconvolved FWHM Location size in mass vs. size diagram, consistent with BE spheroids peak High degree of concentration: N H2 /<N H2 > ~ 4 on average Median column density contrast over the background ~ 1.5 Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
11 Polaris: `Compact Source Extraction (using getsources A. Menshchikov et al. 2010) Herschel (SPIRE+PACS) Column density map (H 2 /cm 2 ) Spatial distribution of ~ 300 extracted cores (all starless) + galaxies (!) deg ~ 2.6 pc 160/250/500 µm composite image Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
12 Most of the Polaris starless cores are unbound Motte et al. (2001) Mass, M (M ) Cirrus noise limit in Polaris not (yet?) prestellar André et al Ward-Thompson et al Talk by D. Ward-Thompson on Wednesday Deconvolved FWHM size Location in mass vs. size diagram: 2 orders of magnitude below the density of self-gravitating Bonnor-Ebert isothermal spheres Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
13 Confirming the link between the prestellar CMF & the IMF Könyves et al André et al A&A special issue prestellar cores in Aquila Prestellar Core Mass Function (CMF) in Aquila Complex IMF CMF CO clumps (Kramer et al. 1998) Factor ~ 2-9 better statistics than earlier studies: ε Salpeter s IMF e.g. Motte, André, Neri 1998; Johnstone et al. 2000; Beuther & Schilke 2004; Stanke et al. 2006; Enoch et al. 2006; Alves et al. 2007; Nutter & Ward-Thompson 07 Good (~ one-to-one) correspondence between core mass and system mass: M * = ε M core with ε ~ in Aquila The IMF is at least partly determined by pre-collapse cloud fragmentation (cf. models by Padoan & Nordlund 2002, Hennebelle & Chabrier 2008)
14 The Polaris starless cores are not massive enough to form stars Mass Function of the Starless Cores in Polaris IMF CO clumps Salpeter s IMF André et al The mass function of Polaris starless cores peaks at ~ 0.02 M, i.e., ~ one order of magnitude below the peak of the stellar IMF
15 Prestellar cores form out of a filamentary background Herschel (SPIRE+PACS) Column density map (H 2 /cm 2 ) Curvelet component of column density map (H 2 /cm 2 ) Mline/Mline,crit Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
16 : Class 0 protostars Prestellar cores form out of a filamentary background Aquila N H2 map (cm -2 ) : Prestellar cores - 80% found at A v (back) > Aquila curvelet N H2 map (cm -2 ) Mline/Mline,crit Unstable Stable 1 Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
17 Only the densest filaments are gravitationally unstable and contain prestellar cores ( ) Aquila curvelet N H2 map (cm -2 ) André et al. 2010, A&A special issue 1 Unstable Mline/M line,crit 0.1 Stable The gravitational instability of filaments is controlled by the value of their mass per unit length M line (cf. Ostriker 1964, Inutsuka & Miyama 1997): unstable if M line > M line, crit stable if M line < M line, crit M line, crit = c s 2 /G ~ 15 M /pc for T = 10K Simple estimate: M line N H2 x Width Unstable filaments highlighted in white in the N H2 map
18 Polaris (d ~ 150 pc): Structure of the cold ISM prior to any star formation Polaris curvelet N H2 map (cm -2 ) No prestellar cores (yet?) in Polaris 0.5 Filaments are already widespread prior to star formation André et al. 2010, A&A special issue 0.1Mline/Mline,crit 0.01 The maximum value of M line /M line, crit observed in the Polaris filaments is ~ 0.5 The Polaris filaments are gravitationally stable and unable to form prestellar cores and protostars at present
19 Filaments permeate the ISM on all scales Herschel SPIRE 500 µm + PACS 160/70 µm Planck HFI 540/350 µm + IRAS 100 µm Aquila ESA and the Gould Belt KP ESA and the HFI Consortium
20 Conclusions Gould Belt Cepheus Serpens Ophiuchus Lupus Herschel Aquila Main Taurus Perseus Aquila Chamaeleon CrA Orion IRAS 100 µm Our first results are extremely promising; exceed expectations! Confirm the close link between the prestellar CMF and the IMF Suggest an observationally-driven scenario of core formation: 1) Filaments form first in the cold ISM, possibly as a result of interstellar MHD turbulence; 2) The densest filaments then fragment into prestellar cores via gravitational instability. MANY THANKS TO ESA HSC + SPIRE & PACS ICCs Ph. André - ESLAB 2010 Herschel First Results - ESTEC 4 May 2010
NGUYEN LUONG QUANG. Président du jury: J. Le Bourlot Rapporteurs: H. Beuther, T. Moore Examinateurs: I. Bonnell, F. Boulanger, F. Combes, F.
NGUYEN LUONG QUANG Supervisors: Frédérique Motte (CEA Saclay) Marc Sauvage (CEA Saclay) Président du jury: J. Le Bourlot Rapporteurs: H. Beuther, T. Moore Examinateurs: I. Bonnell, F. Boulanger, F. Combes,
IV. Molecular Clouds. 1. Molecular Cloud Spectra
IV. Molecular Clouds Dark structures in the ISM emit molecular lines. Dense gas cools, Metals combine to form molecules, Molecular clouds form. 1. Molecular Cloud Spectra 1 Molecular Lines emerge in absorption:
Resultados Concurso Apex 2014-A
Resultados Concurso Apex 2014-A Propuesta: 2014A/04 Investigador Principal: Guido Garay, Universidad de Chila Título: SuperMALT: determining the physical and chemical evolution of high-mass starforming
Lecture 3 Properties and Evolution of Molecular Clouds. Spitzer space telescope image of Snake molecular cloud (IRDC G11.11-0.11
Lecture 3 Properties and Evolution of Molecular Clouds Spitzer space telescope image of Snake molecular cloud (IRDC G11.11-0.11 From slide from Annie Hughes Review CO t in clouds HI: Atomic Hydrogen http://www.atnf.csiro.au/research/lvmeeting/magsys_pres/
Star Formation in the Large Magellanic Cloud: Tracing an Evolution of Giant Molecular Clouds
Star Formation in the Large Magellanic Cloud: Tracing an Evolution of Giant Molecular Clouds Toshikazu Onishi Osaka Prefecture University Yasuo Fukui; Akiko Kawamura; Norikazu Mizuno; Tetsuhiro Minamidani;
Observing the Universe
Observing the Universe Stars & Galaxies Telescopes Any questions for next Monday? Light Doppler effect Doppler shift Doppler shift Spectra Doppler effect Spectra Stars Star and planet formation Sun Low-mass
The Chemical Composition of a Molecular Cloud at the Outer Edge of the Galaxy
Carnegie Observatories Astrophysics Series, Vol. 4: Origin and Evolution of the Elements, 2003 ed. A. McWilliam and M. Rauch (Pasadena: Carnegie Observatories, http://www.ociw.edu/ociw/symposia/series/symposium4/proceedings.html)
Heating & Cooling in Molecular Clouds
Lecture 8: Cloud Stability Heating & Cooling in Molecular Clouds Balance of heating and cooling processes helps to set the temperature in the gas. This then sets the minimum internal pressure in a core
7. In which part of the electromagnetic spectrum are molecules most easily detected? A. visible light B. radio waves C. X rays D.
1. Most interstellar matter is too cold to be observed optically. Its radiation can be detected in which part of the electromagnetic spectrum? A. gamma ray B. ultraviolet C. infrared D. X ray 2. The space
Nuclear fusion in stars. Collapse of primordial density fluctuations into galaxies and stars, nucleosynthesis in stars
Nuclear fusion in stars Collapse of primordial density fluctuations into galaxies and stars, nucleosynthesis in stars The origin of structure in the Universe Until the time of formation of protogalaxies,
Ellipticals. Elliptical galaxies: Elliptical galaxies: Some ellipticals are not so simple M89 E0
Elliptical galaxies: Ellipticals Old view (ellipticals are boring, simple systems)! Ellipticals contain no gas & dust! Ellipticals are composed of old stars! Ellipticals formed in a monolithic collapse,
L3: The formation of the Solar System
credit: NASA L3: The formation of the Solar System UCL Certificate of astronomy Dr. Ingo Waldmann A stable home The presence of life forms elsewhere in the Universe requires a stable environment where
Class 2 Solar System Characteristics Formation Exosolar Planets
Class 1 Introduction, Background History of Modern Astronomy The Night Sky, Eclipses and the Seasons Kepler's Laws Newtonian Gravity General Relativity Matter and Light Telescopes Class 2 Solar System
Gamma Rays from Molecular Clouds and the Origin of Galactic Cosmic Rays. Stefano Gabici APC, Paris
Gamma Rays from Molecular Clouds and the Origin of Galactic Cosmic Rays Stefano Gabici APC, Paris The Origin of galactic Cosmic Rays Facts: the spectrum is (ALMOST) a single power law -> CR knee at few
Modeling Galaxy Formation
Galaxy Evolution is the study of how galaxies form and how they change over time. As was the case with we can not observe an individual galaxy evolve but we can observe different galaxies at various stages
The Solar Journey: Modeling Features of the Local Bubble and Galactic Environment of the Sun
The Solar Journey: Modeling Features of the Local Bubble and Galactic Environment of the Sun P.C. Frisch and A.J. Hanson Department of Astronomy and Astrophysics University of Chicago and Computer Science
In studying the Milky Way, we have a classic problem of not being able to see the forest for the trees.
In studying the Milky Way, we have a classic problem of not being able to see the forest for the trees. A panoramic painting of the Milky Way as seen from Earth, done by Knut Lundmark in the 1940 s. The
Lesson 3: Isothermal Hydrostatic Spheres. B68: a self-gravitating stable cloud. Hydrostatic self-gravitating spheres. P = "kt 2.
Lesson 3: Isothermal Hydrostatic Spheres B68: a self-gravitating stable cloud Bok Globule Relatively isolated, hence not many external disturbances Though not main mode of star formation, their isolation
Gravitational instabilities in protostellar discs and the formation of planetesimals
Gravitational instabilities in protostellar discs and the formation of planetesimals Giuseppe Lodato - Università degli Studi di Milano 17 February 2011 - Bologna Gravitational instabilities in protostellar
Lecture 6: distribution of stars in. elliptical galaxies
Lecture 6: distribution of stars in topics: elliptical galaxies examples of elliptical galaxies different classes of ellipticals equation for distribution of light actual distributions and more complex
A Universe of Galaxies
A Universe of Galaxies Today s Lecture: Other Galaxies (Chapter 16, pages 366-397) Types of Galaxies Habitats of Galaxies Dark Matter Other Galaxies Originally called spiral nebulae because of their shape.
Star Clusters. Star Clusters E NCYCLOPEDIA OF A STRONOMY AND A STROPHYSICS
Star Clusters Even a small telescope shows obvious local concentrations of stars scattered around the sky. These star clusters are not chance juxtapositions of unrelated stars. They are, instead, physically
Malcolm S. Longair. Galaxy Formation. With 141 Figures and 12 Tables. Springer
Malcolm S. Longair Galaxy Formation With 141 Figures and 12 Tables Springer Contents Part I Preliminaries 1. Introduction, History and Outline 3 1.1 Prehistory 3 1.2 The Theory of the Expanding Universe
Detailed Mass Map of CL 0024+1654 from Strong Lensing
Detailed Mass Map of CL 0024+1654 from Strong Lensing Tyson, Kochanski, & Dell Antonio (1998) HST WFPC2 image of CL0024+1654 slides based on presentation by Yue Zhao Rutgers Physics 690 February 21, 2008
8.1 Radio Emission from Solar System objects
8.1 Radio Emission from Solar System objects 8.1.1 Moon and Terrestrial planets At visible wavelengths all the emission seen from these objects is due to light reflected from the sun. However at radio
Solar Nebula Theory. Basic properties of the Solar System that need to be explained:
Solar Nebula Theory Basic properties of the Solar System that need to be explained: 1. All planets orbit the Sun in the same direction as the Sun s rotation 2. All planetary orbits are confined to the
Using Photometric Data to Derive an HR Diagram for a Star Cluster
Using Photometric Data to Derive an HR Diagram for a Star Cluster In In this Activity, we will investigate: 1. How to use photometric data for an open cluster to derive an H-R Diagram for the stars and
Faber-Jackson relation: Fundamental Plane: Faber-Jackson Relation
Faber-Jackson relation: Faber-Jackson Relation In 1976, Faber & Jackson found that: Roughly, L! " 4 More luminous galaxies have deeper potentials Can show that this follows from the Virial Theorem Why
The Interstellar Medium Astronomy 216 Spring 2005
The Interstellar Medium Astronomy 216 Spring 2005 Al Glassgold & James Graham University of California, Berkeley The Interstellar Medium/Media (ISM) What is the ISM? Just what it says: The stuff between
Class #14/15 14/16 October 2008
Class #14/15 14/16 October 2008 Thursday, Oct 23 in class You ll be given equations and constants Bring a calculator, paper Closed book/notes Topics Stellar evolution/hr-diagram/manipulate the IMF ISM
Activity: Multiwavelength Bingo
ctivity: Multiwavelength background: lmost everything that we know about distant objects in the Universe comes from studying the light that is emitted or reflected by them. The entire range of energies
Adaptive Optics (AO) TMT Partner Institutions Collaborating Institution Acknowledgements
THIRTY METER TELESCOPE The past century of astronomy research has yielded remarkable insights into the nature and origin of the Universe. This scientific advancement has been fueled by progressively larger
Exceptionally massive and bright, the earliest stars changed the course of cosmic history
THE FIRST STARS IN THE UNIVERSE Exceptionally massive and bright, the earliest stars changed the course of cosmic history BY RICHARD B. LARSON AND VOLKER BROMM ILLUSTRATIONS BY DON DIXON We live in a universe
Sound. References: L.D. Landau & E.M. Lifshitz: Fluid Mechanics, Chapter VIII F. Shu: The Physics of Astrophysics, Vol. 2, Gas Dynamics, Chapter 8
References: Sound L.D. Landau & E.M. Lifshitz: Fluid Mechanics, Chapter VIII F. Shu: The Physics of Astrophysics, Vol., Gas Dynamics, Chapter 8 1 Speed of sound The phenomenon of sound waves is one that
ENERGY TRANSPORT WITHIN A STAR
M. Pettini: Structure and Evolution of Stars Lecture 8 ENERGY TRANSPORT WITHIN A STAR 8.1 Introduction Up to now, we have considered how energy is generated within the interior of stars by the processes
Lecture 19: Planet Formation I. Clues from the Solar System
Lecture 19: Planet Formation I. Clues from the Solar System 1 Outline The Solar System:! Terrestrial planets! Jovian planets! Asteroid belt, Kuiper belt, Oort cloud Condensation and growth of solid bodies
Planck Early Results: New light on Anomalous Microwave Emission from Spinning Dust Grains
Planck Early Results: New light on Anomalous Microwave Emission from Spinning Dust Grains Perseus in the optical Clive Dickinson Jodrell Bank Centre for Astrophysics (University of Manchester) On behalf
Astronomy & Physics Resources for Middle & High School Teachers
Astronomy & Physics Resources for Middle & High School Teachers Gillian Wilson http://www.faculty.ucr.edu/~gillianw/k12 A cosmologist is.... an astronomer who studies the formation and evolution of the
Summary: Four Major Features of our Solar System
Summary: Four Major Features of our Solar System How did the solar system form? According to the nebular theory, our solar system formed from the gravitational collapse of a giant cloud of interstellar
Evolution of Close Binary Systems
Evolution of Close Binary Systems Before going on to the evolution of massive stars and supernovae II, we ll think about the evolution of close binary systems. There are many multiple star systems in the
Elliptical Galaxies. Houjun Mo. April 19, 2004. Basic properties of elliptical galaxies. Formation of elliptical galaxies
Elliptical Galaxies Houjun Mo April 19, 2004 Basic properties of elliptical galaxies Formation of elliptical galaxies Photometric Properties Isophotes of elliptical galaxies are usually fitted by ellipses:
Lecture 7 Formation of the Solar System. Nebular Theory. Origin of the Solar System. Origin of the Solar System. The Solar Nebula
Origin of the Solar System Lecture 7 Formation of the Solar System Reading: Chapter 9 Quiz#2 Today: Lecture 60 minutes, then quiz 20 minutes. Homework#1 will be returned on Thursday. Our theory must explain
on Recent Developments on Theoretical and Experimental General Relativity, Astrophysics, and Relativistic Field Theories
Thirteenth Marcel Grossman Meeting on Recent Developments on Theoretical and Experimental General Relativity, Astrophysics, and Relativistic Field Theories ON GENERAL RELATIVISTIC UNIFORMLY ROTATING WHITE
The Birth and Assembly of Galaxies: the Relationship Between Science Capabilities and Telescope Aperture
The Birth and Assembly of Galaxies: the Relationship Between Science Capabilities and Telescope Aperture Betsy Barton Center for Cosmology University of California, Irvine Grateful acknowledgements to:
The Hidden Lives of Galaxies. Jim Lochner, USRA & NASA/GSFC
The Hidden Lives of Galaxies Jim Lochner, USRA & NASA/GSFC What is a Galaxy? Solar System Distance from Earth to Sun = 93,000,000 miles = 8 light-minutes Size of Solar System = 5.5 light-hours What is
Explain the Big Bang Theory and give two pieces of evidence which support it.
Name: Key OBJECTIVES Correctly define: asteroid, celestial object, comet, constellation, Doppler effect, eccentricity, eclipse, ellipse, focus, Foucault Pendulum, galaxy, geocentric model, heliocentric
Study Guide: Solar System
Study Guide: Solar System 1. How many planets are there in the solar system? 2. What is the correct order of all the planets in the solar system? 3. Where can a comet be located in the solar system? 4.
THE HR DIAGRAM THE MOST FAMOUS DIAGRAM in ASTRONOMY Mike Luciuk
THE HR DIAGRAM THE MOST FAMOUS DIAGRAM in ASTRONOMY Mike Luciuk 1.INTRODUCTION Late in the nineteenth century, astronomers had tools that revealed a great deal about stars. By that time, advances in telescope
SLAS Messier Marathon Log Sheets # Messier Constellation Type Rating Instrument Date Time Location 1 M77 Cetus Galaxy Difficult
1 M77 Cetus Galaxy Difficult 2 M74 Pisces Galaxy Difficult 3 M33 Triangulum Galaxy Difficult 4 M31 Andromeda Galaxy Easy 5 M32 Andromeda Galaxy Difficult 6 M110 Andromeda Galaxy Difficult 7 M52 Cassiopeia
1. Degenerate Pressure
. Degenerate Pressure We next consider a Fermion gas in quite a different context: the interior of a white dwarf star. Like other stars, white dwarfs have fully ionized plasma interiors. The positively
Populations and Components of the Milky Way
Chapter 2 Populations and Components of the Milky Way Our perspective from within the Milky Way gives us an opportunity to study a disk galaxy in detail. At the same time, it s not always easy to relate
13 Space Photos To Remind You The Universe Is Incredible
13 Space Photos To Remind You The Universe Is Incredible NASA / Via photojournal.jpl.nasa.gov New ultraviolet images from NASA s Galaxy Evolution Explorer shows a speeding star that is leaving an enormous
8 Radiative Cooling and Heating
8 Radiative Cooling and Heating Reading: Katz et al. 1996, ApJ Supp, 105, 19, section 3 Thoul & Weinberg, 1995, ApJ, 442, 480 Optional reading: Thoul & Weinberg, 1996, ApJ, 465, 608 Weinberg et al., 1997,
165 points. Name Date Period. Column B a. Cepheid variables b. luminosity c. RR Lyrae variables d. Sagittarius e. variable stars
Name Date Period 30 GALAXIES AND THE UNIVERSE SECTION 30.1 The Milky Way Galaxy In your textbook, read about discovering the Milky Way. (20 points) For each item in Column A, write the letter of the matching
astronomy 2008 1. A planet was viewed from Earth for several hours. The diagrams below represent the appearance of the planet at four different times.
1. A planet was viewed from Earth for several hours. The diagrams below represent the appearance of the planet at four different times. 5. If the distance between the Earth and the Sun were increased,
FXA 2008. UNIT G485 Module 5 5.5.1 Structure of the Universe. Δλ = v λ c CONTENTS OF THE UNIVERSE. Candidates should be able to :
1 Candidates should be able to : CONTENTS OF THE UNIVERSE Describe the principal contents of the universe, including stars, galaxies and radiation. Describe the solar system in terms of the Sun, planets,
Answers for the Student Worksheet for the Hubble Space Telescope Scavenger Hunt
Instructions: Answers are typed in blue. Answers for the Student Worksheet for the Hubble Space Telescope Scavenger Hunt Crab Nebula What is embedded in the center of the nebula? Neutron star Who first
UNIT V. Earth and Space. Earth and the Solar System
UNIT V Earth and Space Chapter 9 Earth and the Solar System EARTH AND OTHER PLANETS A solar system contains planets, moons, and other objects that orbit around a star or the star system. The solar system
