A Comprehensive View of the Virgo Stellar Stream?,??
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Arxiv:Astro-Ph/0609104V2 31 Jan 2007
Draft version July 23, 2018 A Preprint typeset using LTEX style emulateapj v. 08/22/09 THE VIRGO STELLAR OVER-DENSITY: MAPPING THE INFALL OF THE SAGITTARIUS TIDAL STREAM ONTO THE MILKY WAY DISK David Mart´ınez-Delgado1,2, Jorge Penarrubia˜ 3,4, Mario Juric´5,6, Emilio J. Alfaro2, Zeljko Ivezic´5 Draft version July 23, 2018 ABSTRACT The recently discovered Virgo stellar over-density, which expands over 1000deg2 perpendicularly to the Galactic disk plane (7<Z < 15 kpc, R 7 kpc), is the largest∼ clump of tidal debris ever detected in the outer halo and is likely related with∼ the accretion of a nearby dwarf galaxy by the Milky Way. We carry out N-body simulations of the Sagittarius stream to show that this giant stellar over-density is a confirmation of theoretical model predictions for the leading tail of the Sagittarius stream to cross the Milky Way plane in the Solar neighborhood. Radial velocity measurements are needed to confirm this association and to further constrain the shape of the Milky Way dark matter halo through a new generation of theoretical models. If the identification of Virgo over-density and the Sagittarius leading arm is correct, we predict highly negative radial velocities for the stars of Virgo over-density. The detection of this new portion of the Sagittarius tidal stream would represent an excellent target for the on-going and future kinematic surveys and for dark matter direct detection experiments in the proximity of the Sun. Subject headings: galaxies: individual (Sagittarius) — galaxies:interactions—Galaxy: structure — Galaxy: halo 1. -
Experiencing Hubble
PRESCOTT ASTRONOMY CLUB PRESENTS EXPERIENCING HUBBLE John Carter August 7, 2019 GET OUT LOOK UP • When Galaxies Collide https://www.youtube.com/watch?v=HP3x7TgvgR8 • How Hubble Images Get Color https://www.youtube.com/watch? time_continue=3&v=WSG0MnmUsEY Experiencing Hubble Sagittarius Star Cloud 1. 12,000 stars 2. ½ percent of full Moon area. 3. Not one star in the image can be seen by the naked eye. 4. Color of star reflects its surface temperature. Eagle Nebula. M 16 1. Messier 16 is a conspicuous region of active star formation, appearing in the constellation Serpens Cauda. This giant cloud of interstellar gas and dust is commonly known as the Eagle Nebula, and has already created a cluster of young stars. The nebula is also referred to the Star Queen Nebula and as IC 4703; the cluster is NGC 6611. With an overall visual magnitude of 6.4, and an apparent diameter of 7', the Eagle Nebula's star cluster is best seen with low power telescopes. The brightest star in the cluster has an apparent magnitude of +8.24, easily visible with good binoculars. A 4" scope reveals about 20 stars in an uneven background of fainter stars and nebulosity; three nebulous concentrations can be glimpsed under good conditions. Under very good conditions, suggestions of dark obscuring matter can be seen to the north of the cluster. In an 8" telescope at low power, M 16 is an impressive object. The nebula extends much farther out, to a diameter of over 30'. It is filled with dark regions and globules, including a peculiar dark column and a luminous rim around the cluster. -
The Search for Transiting Extrasolar Planets in the Open Cluster M52
THE SEARCH FOR TRANSITING EXTRASOLAR PLANETS IN THE OPEN CLUSTER M52 A Thesis Presented to the Faculty of San Diego State University In Partial Fulfillment of the Requirements for the Degree Master of Sciences in Astronomy by Tiffany M. Borders Summer 2008 SAN DIEGO STATE UNIVERSITY The Undersigned Faculty Committee Approves the Thesis of Tiffany M. Borders: The Search for Transiting Extrasolar Planets in the Open Cluster M52 Eric L. Sandquist, Chair Department of Astronomy William Welsh Department of Astronomy Calvin Johnson Department of Physics Approval Date iii Copyright 2008 by Tiffany M. Borders iv DEDICATION To all who seek new worlds. v Success is to be measured not so much by the position that one has reached in life as by the obstacles which he has overcome. –Booker T. Washington All the world’s a stage, And all the men and women merely players. They have their exits and their entrances; And one man in his time plays many parts... –William Shakespeare, “As You Like It”, Act 2 Scene 7 vi ABSTRACT OF THE THESIS The Search for Transiting Extrasolar Planets in the Open Cluster M52 by Tiffany M. Borders Master of Sciences in Astronomy San Diego State University, 2008 In this survey we attempt to discover short-period Jupiter-size planets in the young open cluster M52. Ten nights of R-band photometry were used to search for planetary transits. We obtained light curves of 4,128 stars and inspected them for variability. No planetary transits were apparent; however, some interesting variable stars were discovered. In total, 22 variable stars were discovered of which, 19 were not previously known as variable. -
SATELLITE COMMUNICATION UNIT I OVERVIEW of SATELLITE SYSTEMS, ORBITS and LAUNCHING METHODS Introduction
www.jntuhweb.com JNTUH WEB SATELLITE COMMUNICATION UNIT I OVERVIEW OF SATELLITE SYSTEMS, ORBITS AND LAUNCHING METHODS Introduction – Frequency allocations for satellite services – Intelsat – U.S domsats – Polar orbiting satellites – Problems – Kepler’s first law – Kepler’s second law – Kepler’s third law – Definitions of terms for earth – Orbiting satellites – Orbital elements – Apogee and perigee heights – Orbital perturbations – Effects of a non-spherical earth – Atmospheric drag – Inclined orbits – Calendars – Universal time – Julian dates – Sidereal time – The orbital plane – The geocentric – Equatorial coordinate system – Earth station referred to the IJK frame – The topcentric – Horizon co-ordinate system – The subsatellite point – Predicting satellite position. PART A 1. What is Satellite? Mention the types. An artificial body that is projected from earth to orbit either earth (or) another body of solar systems. Types: Information satellites and Communication Satellites 2. State Kepler’s first law. It states that the path followed by the satellite around the primary will be an ellipse. An ellipse has two focal points F1 and F2. The center of mass of the two body system, termed the barycenter is always centered on one of the foci. e = [square root of ( a2– b2) ] / a 3. State Kepler’s second law. It states that for equal time intervals, the satellite will sweep out equal areas in its orbital Skyupsmediaplane, focused at the barycenter. 4. State Kepler’s third law. It states that the square of the periodic time of orbit is perpendicular to the cube of the mean distance between the two bodies. JNTUH WEB www.jntuhweb.com JNTUH WEB a3= 3 / n2 Where, n = Mean motion of the satellite in rad/sec. -
Rings and Radial Waves in the Disk of the Milky Way Xu, Newberg, Carlin, Liu, Deng, Li, Schönrich & Yanny, Apj, in Press, 2015
Dana Berry Rings and Radial Waves in the Disk of the Milky Way Xu, Newberg, Carlin, Liu, Deng, Li, Schönrich & Yanny, ApJ, in press, 2015 We identify an asymmetry in disk stars that oscillates Xu Yan from the north to the south to the north to the south NAOC, Beijing across the Galactic plane in the anticenter direction. Newberg et al. 2002 ? Monoceros Ring Vivas overdensity, or Virgo Stellar Stream Hercules-Aquila Cloud Stellar Spheroid Sagittarius Dwarf Tidal Stream Monoceros Monoceros (l,b)=(200°, -24°) (l, b) = (123°, -19°) Newberg et al. (2002), Figure 15 Ibata et al. (2003), Figure 6 The early papers differed on the identification of Monoceros in the south, leading to a decade of confusion in the literature. Newberg et al. 2002 Monoceros stream, Stream in the Galactic Plane, ? Galactic Anticenter Stellar Stream, Vivas overdensity, or Canis Major Stream, Virgo Stellar Stream Argo Navis Stream Hercules-Aquila Cloud Stellar Spheroid Sagittarius Dwarf Tidal Stream The SDSS also took imaging (and spectroscopic) data along 2.5°- wide stripes at constant Galactic longitude. These stripes cross the Galactic plane. The SDSS also took imaging (and spectroscopic) data along 2.5°- wide stripes at constant Galactic longitude. These stripes cross the Galactic plane. Counts of Stars with 0.4 < (g −r) < 0.5 Direction of 0 reddening vector Getting the reddening wrong does not change the result. The difference in counts is huge – like a factor of two. Isochrone Fitting (l,b)=(178◦, 15◦) (l,b)=(203◦,−25◦) Isochrones were fit to the north near ([Fe/H]=-0.5), south middle ([Fe/H]=-0.88), Monoceros Ring (M5), and TriAnd Ring (M5), using empirical isochrones from An et al. -
Proper Motions in Kapteyn Selected Area 103: a Preliminary Orbit for The
Proper Motions in Kapteyn Selected Area 103: A Preliminary Orbit for the Virgo Stellar Stream Dana I. Casetti-Dinescu1,2,3, Terrence M. Girard1, Steven R. Majewski4, A. Katherina Vivas5, Ronald Wilhelm6, Jeffrey L. Carlin4, Timothy C. Beers7, and William F. van Altena1 ABSTRACT We present absolute proper motions in Kapteyn Selected Area (SA) 103. This field is located 7◦ west of the center of the Virgo Stellar Stream (VSS, Duffau et al. 2006), and has a well-defined main sequence representing the stream. In SA 103, we identify one RR Lyrae star as a member of the VSS, according to its metallicity, radial velocity, and distance. VSS candidate turnoff and subgiant stars have proper motions consistent with that of the RR Lyrae star. The 3D velocity data imply an orbit with a pericenter of ∼ 11 kpc and an apocenter of ∼ 90 kpc. Thus, the VSS comprises tidal debris found near the pericenter of a highly destructive orbit. Examining the six globular clusters at distances larger than 50 kpc from the Galactic center, and the proposed orbit of the VSS, we find one tentative association, NGC 2419. We speculate that NGC 2419 is possibly the nucleus of a disrupted system of which the VSS is a part. Subject headings: Galaxy: structure — Galaxy: kinematics and dynamics — Galaxy: halo 1Astronomy Department, Yale University, P.O. Box 208101, New Haven, CT 06520-8101, USA 2 arXiv:0907.1249v1 [astro-ph.GA] 7 Jul 2009 Astronomy Department, Van Vleck Observatory, Wesleyan University, Middletown, CT 06459, USA 3Astronomical Institute of the Romanian Academy, Str. Cutitul de Argint 5, RO-75212, Bucharest 28, Romania 4Department of Astronomy, University of Virginia, P.O Box 400325, Charlottesville, VA 22904-4325 5Centro de Investigaciones de Astronomia (CIDA), Apartado Postal 264, M´erida, 5101-A, Venezuela 6Department of Physics, Texas Tech University, Lubbock, TX 79409, USA 7Department of Physics and Astronomy, CSCE: Center for the Study of Cosmic Evolution, and JINA: Joint Institution for Nuclear Astrophysics, Michigan State University, E. -
Lecture 2, Galaxy Number Counts and Luminosity Functions
Galaxies 626 Lecture 2: Galaxy number counts and luminosity functions How much of the extragalactic background light can we identify, and how much is unidentified (unresolved)? The next step is to count all the galaxies we can find and see how much light they contain So we now want to form the galaxy number counts at all wavelengths B, R, z/ 15/ x 15/ B (1.7hrs) R (5.2hrs) z’ (3.9hrs) B (27) R (26.4) z’ (25.4) Optical Image Capak et al. 2003 Measuring Galaxy Luminosities Galaxies, unlike stars, are not point sources The Hubble Space Telescope can resolve (i.e. detect the extended nature of) essentially all galaxies Even from the ground, most galaxies can easily be distinguished from stars morphologically and on the basis of their colors Measuring Galaxy Luminosities Define the surface brightness of a galaxy I as the amount of light from the galaxy per square arcsecond on the sky Consider a small square patch, of side D, in a galaxy at distance d: d D Angle patch subtends on sky α = D/d Finding Galaxies in an Image Finding galaxies in an image and constructing the number counts is the subject of the first student project Essentially we look for all objects above a limiting surface brightness and covering more than a specified area SExtractor is a commonly used package 20 cm Radio Image from the VLA Number Counts We then need to measure the fluxes of all the objects that we find The number counts are simply the number of objects we find in a given flux or magnitude bin per unit area of the sky Measuring Galaxy Luminosities Consider again -
Download This Issue (Pdf)
Volume 46 Number 2 JAAVSO 2018 The Journal of the American Association of Variable Star Observers Unmanned Aerial Systems for Variable Star Astronomical Observations The NASA Altair UAV in flight. Also in this issue... • A Study of Pulsation and Fadings in some R CrB Stars • Photometry and Light Curve Modeling of HO Psc and V535 Peg • Singular Spectrum Analysis: S Per and RZ Cas • New Observations, Period and Classification of V552 Cas • Photometry of Fifteen New Variable Sources Discovered by IMSNG Complete table of contents inside... The American Association of Variable Star Observers 49 Bay State Road, Cambridge, MA 02138, USA The Journal of the American Association of Variable Star Observers Editor John R. Percy Laszlo L. Kiss Ulisse Munari Dunlap Institute of Astronomy Konkoly Observatory INAF/Astronomical Observatory and Astrophysics Budapest, Hungary of Padua and University of Toronto Asiago, Italy Toronto, Ontario, Canada Katrien Kolenberg Universities of Antwerp Karen Pollard Associate Editor and of Leuven, Belgium Director, Mt. John Observatory Elizabeth O. Waagen and Harvard-Smithsonian Center University of Canterbury for Astrophysics Christchurch, New Zealand Production Editor Cambridge, Massachusetts Michael Saladyga Nikolaus Vogt Kristine Larsen Universidad de Valparaiso Department of Geological Sciences, Valparaiso, Chile Editorial Board Central Connecticut State Geoffrey C. Clayton University, Louisiana State University New Britain, Connecticut Baton Rouge, Louisiana Vanessa McBride Kosmas Gazeas IAU Office of Astronomy for University of Athens Development; South African Athens, Greece Astronomical Observatory; and University of Cape Town, South Africa The Council of the American Association of Variable Star Observers 2017–2018 Director Stella Kafka President Kristine Larsen Past President Jennifer L. -
Surface Brightness Profiles
AST222 Winter 2006 Supplementary Notes: Galaxy Surface Brightness Pro¯les The fundamental way we characterize the morphology of galaxies is through their surface brightness pro¯les. The light from galaxies follows a distribution of brightness on the night sky given by I(x; y) where I is the intensity or surface brightness distribution measured in units of luminosity per unit area at position (x; y) where the area is either in physical units (pc2) or an angular area in square arcseconds. The intensity is often represented by a radially-averaged function, I(R). The total luminosity of a galaxy is then just: 1 Ltot = 2¼ I(R)RdR (1) Z0 Astronomers usually quote surface brightness in units of magnitudes per square arcsec denoted by the symbol ¹. The quantity ¹ represents the apparent magnitude of the equivalent total light observed in a square arcsecond at di®erent points in the distribution. It can be related to the physical surface brightness pro¯le through: ¹ = 2:5 log10 I + C (2) ¡ ¡2 If I is measured in L¯ pc then the constant C can be found by going back to the distance modulus formula and determining the amount of light in a square arcsec for a galaxy observed at distance d (in pc) i.e. the light in a sq. arcsec is: L = Id2±2 (3) where ± = 1" = 1=206265 radians. The distance modulus formula is: m = M + 5 log10 d=(1pc) 5 (4) ¡ where M is the absolute magnitude of the star given in terms of the solar absolute magnitude M¯ by: M = 2:5 log10 L=L¯ + M¯ (5) ¡ (M¯ is the absolute magnitude of the sun not to be confused with the solar mass). -
The Number, Luminosity, and Mass Density of Spiral Galaxies As
The numb er luminosity and mass density of spiral galaxies as a function of surface brightness Stacy S McGaugh Institute of Astronomy University of Cambridge Madingley Road Cambridge CB HA ABSTRACT I give analytic expressions for the relative numb er luminosity and mass density of disc galaxies as a function of surface brightness These surface brightness distributions are asymmetric with long tails to lower surface brightnesses This asymmetry induces systematic errors in most determinations of the galaxy luminosity function Galaxies of low surface brightness exist in large numb ers but the additional contribution to the integrated luminosity density is mo dest probably Key words galaxies formation galaxies fundamental parameters galaxies general galaxies luminosity function mass function galaxies spiral galaxies structure Accepted for publication in the Monthly Notices of the Royal Astronomical Society Present address Department of Terrestrial Magnetism Carnegie Institution of Wash ington Broad Branch Road NW Washington DC USA INTRODUCTION The space density of Low Surface Brightness LSB galaxies has long b een a contro versial and confusing sub ject It is basic to our inventory of the contents of the universe and is crucial to many asp ects of extragalactic astronomy For example the density of LSB galaxies has an impact on the luminosity function faint galaxy numb er counts Ly absorption systems and theories of galaxy formation In this pap er I derive analytic expressions which quantify the density of discs of all surface -
The Cosmic Distance Scale • Distance Information Is Often Crucial to Understand the Physics of Astrophysical Objects
The cosmic distance scale • Distance information is often crucial to understand the physics of astrophysical objects. This requires knowing the basic properties of such an object, like its size, its environment, its location in space... • There are essentially two ways to derive distances to astronomical objects, through absolute distance estimators or through relative distance estimators • Absolute distance estimators Objects for whose distance can be measured directly. They have physical properties which allow such a measurement. Examples are pulsating stars, supernovae atmospheres, gravitational lensing time delays from multiple quasar images, etc. • Relative distance estimators These (ultimately) depend on directly measured distances, and are based on the existence of types of objects that share the same intrinsic luminosity (and whose distance has been determined somehow). For example, there are types of stars that have all the same intrinsic luminosity. If the distance to a sample of these objects has been measured directly (e.g. through trigonometric parallax), then we can use these to determine the distance to a nearby galaxy by comparing their apparent brightness to those in the Milky Way. Essentially we use that log(D1/D2) = 1/5 * [(m1 –m2) - (A1 –A2)] where D1 is the distance to system 1, D2 is the distance to system 2, m1 is the apparent magnitudes of stars in S1 and S2 respectively, and A1 and A2 corrects for the absorption towards the sources in S1 and S2. Stars or objects which have the same intrinsic luminosity are known as standard candles. If the distance to such a standard candle has been measured directly, then the relative distances will have been anchored to an absolute distance scale. -
THE ORION NEBULA and ITS ASSOCIATED POPULATION C. R. O'dell
27 Jul 2001 11:9 AR AR137B-04.tex AR137B-04.SGM ARv2(2001/05/10) P1: FRK Annu. Rev. Astron. Astrophys. 2001. 39:99–136 Copyright c 2001 by Annual Reviews. All rights reserved THE ORION NEBULA AND ITS ASSOCIATED POPULATION C. R. O’Dell Department of Physics and Astronomy, Box 1807-B, Vanderbilt University, Nashville, Tennessee 37235; e-mail: [email protected] Key Words gaseous nebulae, star formation, stellar evolution, protoplanetary disks ■ Abstract The Orion Nebula (M 42) is one of the best studied objects in the sky. The advent of multi-wavelength investigations and quantitative high resolution imaging has produced a rapid improvement in our knowledge of what is widely considered the prototype H II region and young galactic cluster. Perhaps uniquely among this class of object, we have a good three dimensional picture of the nebula, which is a thin blister of ionized gas on the front of a giant molecular cloud, and the extremely dense associated cluster. The same processes that produce the nebula also render visible the circumstellar material surrounding many of the pre–main sequence low mass stars, while other circumstellar clouds are seen in silhouette against the nebula. The process of photoevaporation of ionized gas not only determines the structure of the nebula that we see, but is also destroying the circumstellar clouds, presenting a fundamental conundrum about why these clouds still exist. 1. INTRODUCTION Although M 42 is not the largest, most luminous, nor highest surface brightness H II region, it is the H II region that we know the most about.