ASTRO 1050 Rotation, Mass, and Distance Measurements for Galaxies

Total Page:16

File Type:pdf, Size:1020Kb

ASTRO 1050 Rotation, Mass, and Distance Measurements for Galaxies ASTRO 1050 Rotation, Mass, and Distance Measurements for Galaxies ABSTRACT In this lab we will measure the rotation of spiral galaxies by looking at their spectra. We will then use this rotation to estimate the mass of these galaxies. With this we can also find the mass to light ratios of these galaxies and find that there is dark matter in most galaxies we can see. Measuring the rotation of a Galaxy In this section, we will use the doppler shift of an emission line in a galaxy to measure how it is rotating. To do this, we need to use the doppler shift of light. As objects emitting light get closer to us, the light waves they emit are compressed and shorter and they look bluer. And, as objects move away from us, the light waves they emit are stretched and they look redder. See the image below for a visual representation of this: First, for practice, look at the spectra of the star below. Is it moving towards us, or away from us? How can you tell? 1 Now, we are going to make things more complicated. With an edge-on rotating galaxy, some of the stars are moving towards us and some are moving away from us. This means some of the light is blue shifted, and some is red shifted. If an astronomer measures the spectrum of an entire edge on galaxy, they will see a wider line. We will measure the rotation of galaxy UGC 2936, shown below. Why is this a good candidate for this type of measurement? Now, our helpful observer friend has gone out and taken the spectra of this galaxy, getting light along the blue-green light shown in the following image. The spectra they got is shown below. In this image, instead of looking at wavelength versus intensity, we are measuring wavelength vs. position on this blue line. Our friend has already converted the y-axis to kiloparsecs from the center of the galaxy. They did leave the x axis in angstroms though, which are a unit astronomers use. There are 1010 2 angstroms in one meter (or, 1 angstrom =10−10 meters). Using this spectra, what part of the galaxy is rotating towards us? Which is moving away? In order to find the rotation velocity, we need to measure the difference between the ends of the lines extending off the middle bulge. Using this spectra, what is the shift in wavelength from one end of the galaxy to the other? We also need to know the rest wavelength for this line. For this measurement, we will need to measure the wavelength of this line in the center of the galaxy. What is this measurement? 3 Now, use your two measurements to find the rotational velocity of this galaxy. This can be found using the equation: c∆λ vrot = λrest 8 where vrot is the rotational velocity, c is the speed of light (3 × 10 meters/second), ∆λ is the wavelength shift you measured, and λrest is the rest wavelength you measured. 4 Finding the mass of galaxies from rotational velocity Now, we will look at the measurements from a few edge-on spirals to see how mass is related to rotational velocity. Plot the following measurements in rotational velocity and mass on the graph below. Galaxy Name Mass (solar masses) rotational velocity (km/s) Needle Galaxy 30 × 109 254 NGC 672 8 × 109 143 NGC 925 17 × 109 132 NGC 4559 8 × 109 135 NGC 4631 6 × 109 154 NGC 4656 2 × 109 85 Table 1: Data taken from \Rotation curves, mass distributions and total masses of some spiral galaxies" by N. Krumm and E.E. Salpeter 5 Connect these data points with a line, as best you can. Where would UGC 2936 fall on this graph? Use this to estimate the mass of UGC 2936. 6 Type Ia Supernova We can determine the distance to a galaxy by using the brightness of a type Ia supernova in the galaxy. Below is a list of type Ia supernova and the galaxies they occurred in. Which galaxy is the closest to us? Hint: remember, magnitudes are backwards! Lower magnitude means brighter source Supernova Name Galaxy Supernova Was Observed In Supernova Apparent Magnitude SN 1937C IC 4182 +8.4 SN 1972E NGC 4526 +8.7 SN 1994D NGC 4526 +15.2 SN 2002bi NGC 1821 +14.7 SN 2011fe M101 +10.0 SN 2014J M82 +10.5 Table 2: Data taken from the International Astronomical Union Since we know all Type Ia Supernova have the same absolute magnitude (-19.3) we can find the distance to this nearest galaxy using the formula: m+5=M d = 10 5 where d is the distance to the galaxy, m is the apparent magnitude, and M is the absolute magnitude. 7 Why can we not use Type II supernova (core collapse of a massive star) to find the distance to galaxies? These are some of the ways astronomers can learn about galaxies. Even though they are incredibly distant, we can still find out a lot about them with just a few measurements! 8.
Recommended publications
  • Spiral Galaxy HI Models, Rotation Curves and Kinematic Classifications
    Spiral galaxy HI models, rotation curves and kinematic classifications Theresa B. V. Wiegert A thesis submitted to the Faculty of Graduate Studies of The University of Manitoba in partial fulfillment of the requirements of the degree of Doctor of Philosophy Department of Physics & Astronomy University of Manitoba Winnipeg, Canada 2010 Copyright (c) 2010 by Theresa B. V. Wiegert Abstract Although galaxy interactions cause dramatic changes, galaxies also continue to form stars and evolve when they are isolated. The dark matter (DM) halo may influence this evolu- tion since it generates the rotational behaviour of galactic disks which could affect local conditions in the gas. Therefore we study neutral hydrogen kinematics of non-interacting, nearby spiral galaxies, characterising their rotation curves (RC) which probe the DM halo; delineating kinematic classes of galaxies; and investigating relations between these classes and galaxy properties such as disk size and star formation rate (SFR). To generate the RCs, we use GalAPAGOS (by J. Fiege). My role was to test and help drive the development of this software, which employs a powerful genetic algorithm, con- straining 23 parameters while using the full 3D data cube as input. The RC is here simply described by a tanh-based function which adequately traces the global RC behaviour. Ex- tensive testing on artificial galaxies show that the kinematic properties of galaxies with inclination > 40 ◦, including edge-on galaxies, are found reliably. Using a hierarchical clustering algorithm on parametrised RCs from 79 galaxies culled from literature generates a preliminary scheme consisting of five classes. These are based on three parameters: maximum rotational velocity, turnover radius and outer slope of the RC.
    [Show full text]
  • CONSTELLATION TRIANGULUM, the TRIANGLE Triangulum Is a Small Constellation in the Northern Sky
    CONSTELLATION TRIANGULUM, THE TRIANGLE Triangulum is a small constellation in the northern sky. Its name is Latin for "triangle", derived from its three brightest stars, which form a long and narrow triangle. Known to the ancient Babylonians and Greeks, Triangulum was one of the 48 constellations listed by the 2nd century astronomer Ptolemy. The celestial cartographers Johann Bayer and John Flamsteed catalogued the constellation's stars, giving six of them Bayer designations. The white stars Beta and Gamma Trianguli, of apparent magnitudes 3.00 and 4.00, respectively, form the base of the triangle and the yellow-white Alpha Trianguli, of magnitude 3.41, the apex. Iota Trianguli is a notable double star system, and there are three star systems with planets located in Triangulum. The constellation contains several galaxies, the brightest and nearest of which is the Triangulum Galaxy or Messier 33—a member of the Local Group. The first quasar ever observed, 3C 48, also lies within Triangulum's boundaries. HISTORY AND MYTHOLOGY In the Babylonian star catalogues, Triangulum, together with Gamma Andromedae, formed the constellation known as MULAPIN "The Plough". It is notable as the first constellation presented on (and giving its name to) a pair of tablets containing canonical star lists that were compiled around 1000 BC, the MUL.APIN. The Plough was the first constellation of the "Way of Enlil"—that is, the northernmost quarter of the Sun's path, which corresponds to the 45 days on either side of summer solstice. Its first appearance in the pre-dawn sky (heliacal rising) in February marked the time to begin spring ploughing in Mesopotamia.
    [Show full text]
  • Deep Submillimeter Images of NGC 7331; Dust at the Periphery of Spiral Disks
    A&A 366, 451–465 (2001) Astronomy DOI: 10.1051/0004-6361:20000405 & c ESO 2001 Astrophysics Deep submillimeter images of NGC 7331; dust at the periphery of spiral disks P. B. Alton1, J. Lequeux2, S. Bianchi3, D. Churches1,J.Davies1, and F. Combes2 1 Department of Physics & Astronomy, University of Wales, PO Box 913, Cardiff CF2 3YB, UK 2 DEMIRM, Observatoire de Paris, 61 avenue de l’Observatoire, 75014 Paris, France 3 ESO, Karl-Schwarzschild-Strasse 2, 85748 Garching bei Muenchen, Germany Received 11 September 2000 / Accepted 29 November 2000 Abstract. We present deep 450 and 850 µm SCUBA images of the nearby spiral galaxy NGC 7331. Using the submillimeter emissivity inferred from COBE observations of Milky Way dust, we convert our SCUBA images into maps of optical depth. The opacity derived in this way is quite low at the visible limit of NGC 7331 (τB ≤ 0.22 at the R25 radius for the disk seen face-on). In a similar fashion, we exploit SCUBA and ISOPHOT images of a further 10 galaxies and, collectively, these data indicate τB =0.1–0.2attheR25 radius. Our constraints on disk opacity are fed into a simulation of how light emanating from high redshifts is attenuated by foreground spirals. In making this calculation, we consider the possibility that galactic disks may have also contained different dust masses in the past. We estimate that less than 10% of the light emitted by Hubble Deep Field galaxies fails to reach the B-band observer due to intervening spirals. Key words. ISM: dust, extinction – ISM: molecules – galaxies: spiral – galaxies: ISM – infrared: galaxies – galaxies: NGC 7331 1.
    [Show full text]
  • Cold Gas and Baryon-Induced Dark Matter Cores in Nearby Galaxies
    Cold gas and baryon-induced dark matter cores in nearby galaxies Flor Allaert Supervisors: Prof. Dr. Maarten Baes, Dr. Gianfranco Gentile A dissertation submitted to Ghent University in partial fulfilment of the requirements for the degree of Doctor of Science: Astronomy September 2017 Supervisors: Prof. Dr. Maarten Baes Vakgroep Fysica en Sterrenkunde Universiteit Gent Dr. Gianfranco Gentile Vakgroep Fysica en Sterrenkunde Vrije Universiteit Brussel Jury members: Prof. Dr. Dirk Poelman (President) Vakgroep Vastestofwetenschappen Universiteit Gent Dr. Karel Van Acoleyen (Secretary) Vakgroep Fysica en Sterrenkunde Universiteit Gent Prof. Dr. Sven De Rijcke Vakgroep Fysica en Sterrenkunde Universiteit Gent Prof. Dr. Herwig Dejonghe Vakgroep Fysica en Sterrenkunde Universiteit Gent Prof. Dr. Uli Klein Argelander-Institut fur¨ Astronomie Universitat¨ Bonn Prof. Dr. Erwin de Blok Netherlands Institute for Radio Astronomy Contents 1 Introduction1 1.1 Galaxies - building blocks of the Universe.................1 1.1.1 Classification............................2 1.1.2 Chemical evolution.........................4 1.1.3 Accretion and mergers.......................6 1.2 Observing the different components....................8 1.2.1 Stars................................8 1.2.2 Gas.................................9 1.2.3 Dust................................. 12 1.3 Panchromatic SED modelling and dust radiative transfer......... 13 1.3.1 SED fitting............................. 13 1.3.2 Dust radiative transfer....................... 14 1.3.3 The energy balance problem.................... 15 1.4 FRIEDL, HEROES and NHEMESES................... 17 1.4.1 The energy balance problem revisited............... 18 1.5 Dark matter................................. 18 1.5.1 History............................... 19 1.5.2 Dark matter in cosmology..................... 21 1.5.3 Cosmological simulations..................... 23 1.5.4 The cusp-core controversy..................... 24 1.5.5 Baryons to the rescue?......................
    [Show full text]
  • NIR Counterparts to Ulxs (III): Completing the Photometric Survey and  Selected Spectroscopic Results
    MNRAS 497, 917–932 (2020) doi:10.1093/mnras/staa1920 Advance Access publication 2020 July 7 NIR counterparts to ULXs (III): completing the photometric survey and selected spectroscopic results K. M. Lopez´ ,1,2† M. Heida ,3,4 P. G. Jonker,1,2† M. A. P. Torres,1,5,6 T. P. Roberts,7 D. J. Walton ,8 D.-S. Moon9 and F. A. Harrison4 Downloaded from https://academic.oup.com/mnras/article/497/1/917/5868255 by California Institute of Technology user on 22 October 2020 1SRON Netherlands Institute for Space Research, NL-3584 CA Utrecht, the Netherlands 2Department of Astrophysics/IMAPP, Radboud University, PO Box 9010, NL-6500 GL Nijmegen, the Netherlands 3European Southern Observatory, Karl-Schwarzschild-Straße 2, D-85748 Garching bei Munchen,¨ Germany 4Space Radiation Laboratory, California Institute of Technology, Pasadena, CA 91125, USA 5Instituto de Astrof´ısica de Canarias, E-38200 La Laguna, Tenerife, Spain 6Departamento de Astrof´ısica, Universidad de La Laguna, Astrof´ısico Francisco Sanchez´ S/N, E-38206 La Laguna, Tenerife, Spain 7Centre for Extragalactic Astronomy, Department of Physics, University of Durham, South Road, Durham DH1 3LE, UK 8Institute of Astronomy, Cambridge University, Madingley Road, Cambridge CB3 0HA, UK 9Department of Astronomy and Astrophysics, University of Toronto, Toronto, ON M5S 3H4, Canada Accepted 2020 May 31. Received 2020 May 27; in original form 2019 October 29 ABSTRACT We present results from the remaining sources in our search for near-infrared (NIR) candidate counterparts to ultraluminous X-ray sources (ULXs) within 10 Mpc. We observed 23 ULXs in 15 galaxies and detected NIR candidate counterparts to 6 of them.
    [Show full text]
  • Arxiv:Astro-Ph/0002111V1 4 Feb 2000
    Comparing Galaxy Morphology at Ultraviolet and Optical Wavelengths L. E. Kuchinski1, W. L. Freedman2, Barry F. Madore1,2, M. Trewhella1, R. C. Bohlin3, R. H. Cornett4, M. N. Fanelli4,5, P. M. Marcum6, S. G. Neff7, R. W. O’Connell8, M. S. Roberts9, A. M. Smith7, T. P. Stecher7, W. H. Waller4,10 ABSTRACT We have undertaken an imaging survey of 34 nearby galaxies in far–ultraviolet (FUV, ∼ 1500˚A) and optical (UBV RI) passbands to characterize galaxy morphology as a function of wavelength. This sample, which includes a range of classical Hubble types from elliptical to irregular with emphasis on spirals at low inclination angle, provides a valuable database for comparison with images of high–z galaxies whose FUV light is redshifted into the optical and near–infrared bands. Ultraviolet data are from the UIT Astro–2 mission. We present images and surface brightness profiles for each galaxy, and we discuss the wavelength–dependence of morphology for different Hubble types in the context of understanding high–z objects. In general, the dominance of young stars in the FUV produces the patchy appearance of a morphological type later than that inferred from optical images. Prominent rings and circumnuclear star formation regions are clearly evident in FUV images of spirals, while bulges, bars, and old, red stellar disks are faint to invisible at these short wavelengths. However, the magnitude of the change in apparent morphology ranges from dramatic in early–type spirals with prominent optical bulges to slight in late–type spirals and irregulars, in which young stars dominate both the UV and optical emission.
    [Show full text]
  • Download Date 08/10/2021 22:33:47
    Star forming regions and the IMF along the Hubble sequence Item Type text; Dissertation-Reproduction (electronic) Authors Bresolin, Fabio, 1966- Publisher The University of Arizona. Rights Copyright © is held by the author. Digital access to this material is made possible by the University Libraries, University of Arizona. Further transmission, reproduction or presentation (such as public display or performance) of protected items is prohibited except with permission of the author. Download date 08/10/2021 22:33:47 Link to Item http://hdl.handle.net/10150/288720 INFORMATION TO USERS This manuscript has been reproduced from the microfilm master. UMI films the text dvectty fix>m the origiiial or copy submitted. Thus, some thesis and dissertation copies are in typewriter &c^ while others may be from any type of computer printer. The quality of this reprodoction is dependent upon the quality of the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleedthrough, substandard margins, and improper alignment can adverse^ afifect reproduction. In the unlikely event that the author did not send UMI a complete manuscript and there are missing pages, these will be noted. Also, if unauthorized copyright material had to be removed, a note will indicate the deletion. Oversize materials (e.g., maps, drawings, charts) are reproduced by sectioning the original, b^inning at the upper left-hand comer and continuing from left to right in equal sections with small overiaps. Each original is also photographed in one exposure and is included in reduced form at the back of the book. Photographs included in the original manuscript have been reproduced xerographically in this copy.
    [Show full text]
  • Making a Sky Atlas
    Appendix A Making a Sky Atlas Although a number of very advanced sky atlases are now available in print, none is likely to be ideal for any given task. Published atlases will probably have too few or too many guide stars, too few or too many deep-sky objects plotted in them, wrong- size charts, etc. I found that with MegaStar I could design and make, specifically for my survey, a “just right” personalized atlas. My atlas consists of 108 charts, each about twenty square degrees in size, with guide stars down to magnitude 8.9. I used only the northernmost 78 charts, since I observed the sky only down to –35°. On the charts I plotted only the objects I wanted to observe. In addition I made enlargements of small, overcrowded areas (“quad charts”) as well as separate large-scale charts for the Virgo Galaxy Cluster, the latter with guide stars down to magnitude 11.4. I put the charts in plastic sheet protectors in a three-ring binder, taking them out and plac- ing them on my telescope mount’s clipboard as needed. To find an object I would use the 35 mm finder (except in the Virgo Cluster, where I used the 60 mm as the finder) to point the ensemble of telescopes at the indicated spot among the guide stars. If the object was not seen in the 35 mm, as it usually was not, I would then look in the larger telescopes. If the object was not immediately visible even in the primary telescope – a not uncommon occur- rence due to inexact initial pointing – I would then scan around for it.
    [Show full text]
  • Arxiv:1911.08543V1 [Astro-Ph.GA] 19 Nov 2019 Tions (Diemand Et Al
    MNRAS 000,1{ ?? (2018) Preprint 21 November 2019 Compiled using MNRAS LATEX style file v3.0 The Smallest Scale of Hierarchy Survey (SSH). I. Survey Description. F. Annibali,1? G. Beccari,2 M. Bellazzini,1 M. Tosi,1 F. Cusano,1 D. Paris,5 M. Cignoni,3 L. Ciotti,4 C. Nipoti4 E. Sacchi.6 1INAF - Osservatorio di Astrofisica e Scienza dello Spazio, Via Piero Gobetti, 93/3, I-40129 - Bologna, Italy 2ESO, Karl-Schwarzschild Strasse 2, D-80 Garching, Germany 3Dipartimento di Fisica, Universit`adi Pisa, Largo Bruno Pontecorvo 3, I-56127 Pisa, Italy 4Dipartimento di Fisica e Astronomia, Universit`adi Bologna, via Piero Gobetti 93/2, I-40129 - Bologna, Italy 5INAF-Osservatorio Astronomico di Roma, Via Frascati 33, I-00078 Monte Porzio, Italy 6Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218, USA Accepted XXX. Received YYY; in original form ZZZ ABSTRACT The Smallest Scale of Hierarchy (SSH) survey is an ongoing strategic large program at the Large Binocular Telescope, aimed at the detection of faint stellar streams and satellites around 45 late-type dwarf galaxies located in the Local Universe within '10 Mpc. SSH exploits the wide-field, deep photometry provided by the Large Binocular Cameras in the two wide filters g and r. This paper describes the survey, its goals, and the observational and data reduction strategies. We present preliminary scientific results for five representative cases (UGC 12613, NGC 2366, UGC 685, NGC 5477 and UGC 4426) covering the whole distance range spanned by the SSH targets. We reach a surface brightness limit as faint as µ(r) ∼ 31 mag arcsec−2 both for targets closer than 4−5 Mpc, which are resolved into individual stars, and for more distant targets through the diffuse light.
    [Show full text]
  • A Slow Bar in the Dwarf Irregular Galaxy NGC 3741
    Mon. Not. R. Astron. Soc. 000, 000{000 (0000) Printed 31 October 2018 (MN LATEX style file v2.2) A slow bar in the dwarf irregular galaxy NGC 3741 Arunima Banerjee?, Narendra Nath Patra?, Jayaram N. Chengalur? and Ayesha Begum ?National Centre for Radioy Astrophysics, TIFR, Pune - 411007, India yIndian Institute of Science Education and Research, Bhopal - 462023, India 31 October 2018 ABSTRACT Using the Tremaine-Weinberg method, we measure the speed of the HI bar seen in the disk of NGC 3741. NGC 3741 is an extremely gas rich galaxy with an H i disk which extends to about 8.3 times its Holmberg radius. It is also highly dark matter- −1 −1 dominated. Our calculated value of the pattern speed Ωp is 17.1 3.4 km s kpc . We also find the ratio of the co-rotation radius to the bar semi-major± axis to be (1.6 0.3), indicating a slow bar. This is consistent with bar models in which dynamical friction± results in a slow bar in dark matter dominated galaxies. Key words: galaxies: dwarf - galaxies: irregular - galaxies: ISM - galaxies: kinematics and dynamics - galaxies: structure - galaxies: individual: NGC 3741 1 INTRODUCTION 1999; Debattista et al. 2002; Aguerri et al. 2003; Gressen et al. 2003; Debattista & Williams 2004; Hernandez et al. Understanding the dynamics of galactic bars and its impli- 2005; Emsellem et al. 2006; Corsini et al. 2007; Chemin & cations on galaxy evolution continues to be an important Hernandez 2009; Speights & Westpahl 2012). aspect of studies of galaxy evolution. Bars are found to be present in about half of all disk galaxies (Binney & Tremaine The pattern speed is known to correlate with other pa- 2008).
    [Show full text]
  • New Evidence for Dark Matter
    New evidence for dark matter A. Boyarsky1,2, O. Ruchayskiy1, D. Iakubovskyi2, A.V. Macci`o3, D. Malyshev4 1Ecole Polytechnique F´ed´erale de Lausanne, FSB/ITP/LPPC, BSP CH-1015, Lausanne, Switzerland 2Bogolyubov Institute for Theoretical Physics, Metrologichna str., 14-b, Kiev 03680, Ukraine 3Max-Planck-Institut f¨ur Astronomie, K¨onigstuhl 17, 69117 Heidelberg, Germany 4Dublin Institute for Advanced Studies, 31 Fitzwilliam Place, Dublin 2, Ireland Observations of star motion, emissions from hot ionized gas, gravitational lensing and other tracers demonstrate that the dynamics of galaxies and galaxy clusters cannot be explained by the Newtonian potential produced by visible matter only [1–4]. The simplest resolution assumes that a significant fraction of matter in the Universe, dominating the dynamics of objects from dwarf galaxies to galaxy clusters, does not interact with electromagnetic radiation (hence the name dark matter). This elegant hypothesis poses, however, a major challenge to the highly successful Standard Model of particle physics, as it was realized that dark matter cannot be made of known elementary particles [4]. The quest for direct evidence of the presence of dark matter and for its properties thus becomes of crucial importance for building a fundamental theory of nature. Here we present a new universal relation, satisfied by matter distributions at all observed scales, and show its amaz- ingly good and detailed agreement with the predictions of the most up-to-date pure dark matter simulations of structure formation in the Universe [5–7]. This behaviour seems to be insensitive to the complicated feedback of ordinary matter on dark matter.
    [Show full text]
  • September 1 2 3 4 2021
    Sunday Monday Tuesday Wednesday Thursday Friday Saturday September 1 2 3 4 2021 5 6 7 8 9 10 11 Venus 4.1°S Moon 12 13 14 15 16 17 18 Saturn 3.8°N Moon Jupiter 4.0°N Moon Helix Nebula NGC 7293 19 20 21 22 23 24 25 NASA, ESA, and C.R. O'Dell (Vanderbilt University) 4 Beehive 2.9°S of Moon 6 Mercury at Aphelion 26 27 28 29 30 11 Moon at Perigee: 368464 km 12 Moon at Descending Node 14 Mercury at Greatest Elong: 26.8°E 14 Neptune at Opposition 22 Autumnal Equinox Suggested DSOs for this month 26 Moon at Ascending Node 50mm-500mm 50mm-500mm 135mm-1250mm 135mm-1250mm 200mm-2000mm 300mm-2700mm 750mm-4000mm 26 Moon at Apogee: 404641 km Andromeda Galaxy Elephant Trunk Triangulum Galaxy Pacman Nebula The Hidden Galaxy Sculptor Galaxy Phantom Galaxy 30 Pollux 2.8°N of Moon 420mm-2800mm 700mm-4000mm 50mm-420mm 85mm-600mm 1200mm-4000mm 750mm-4000mm 500mm-4000mm Helix Nebula Dumbbel Nebula Heart Nebula Soul Nebula Nautilus Galaxy Galaxy NGC 891 Barred Spiral Galaxy Credits Andromeda Galaxy M31 All images in this calendar are the property of their respective owners and https://www.astrobin.com/55421/ Raúl López, Skyman have been used either with their permission or respecting their use license. All rights reserved --- The images of Mercury, Venus, Mars, Jupiter, Saturn, Neptune, Uranus and Moon Elephant Trunk IC 1396 https://www.astrobin.com/rl2rcs/ have been obtained from the posters of the "Solar System and Beyond Poster Set" Raúl López, Skyman https://solarsystem.nasa.gov/resources/925/solar-system-and-beyond-poster-set/ All rights reserved --- Triangulum Galaxy M33 The image of the Sun has been obtained from the Solar Dynamics Observatory https://www.flickr.com/photos/rvr/50391788676 https://sdo.gsfc.nasa.gov/ Víctor R.
    [Show full text]