Luminous and Variable Stars in M31 and M33. III. the Yellow and Red Supergiants and Post-Red Supergiant Evolution
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When the Sun Dies, It Will Make
When the Sun dies, it will make: 1. A red giant 2. A planetary nebula 3. A white dwarf 4. A supernova 5. 1, 2, and 3 When the Sun dies, it will make: 1. A red giant 2. A planetary nebula 3. A white dwarf 4. A supernova 5. 1, 2, and 3 A white dwarf star: 1. Is the core of the star from which it formed, and contains most of the mass 2. Is about the size of the earth 3. Is supported by electron degeneracy 4. Is so dense that one teaspoonful would weigh about as much as an elephant 5. All of the above A white dwarf star: 1. Is the core of the star from which it formed, and contains most of the mass 2. Is about the size of the earth 3. Is supported by electron degeneracy 4. Is so dense that one teaspoonful would weigh about as much as an elephant 5. All of the above What keeps a white dwarf from collapsing further? 1. It is solid 2. Electrical forces 3. Chemical forces 4. Nuclear forces 5. Degeneracy pressure What keeps a white dwarf from collapsing further? 1. It is solid 2. Electrical forces 3. Chemical forces 4. Nuclear forces 5. Degeneracy pressure If a white dwarf in a binary has a companion close enough that some material begins to spill onto it, the white dwarf can: 1. Be smothered and cool off 2. Disappear behind the material 3. Have new nuclear reactions and become a nova 4. Become much larger 5. -
Introduction to Astronomy from Darkness to Blazing Glory
Introduction to Astronomy From Darkness to Blazing Glory Published by JAS Educational Publications Copyright Pending 2010 JAS Educational Publications All rights reserved. Including the right of reproduction in whole or in part in any form. Second Edition Author: Jeffrey Wright Scott Photographs and Diagrams: Credit NASA, Jet Propulsion Laboratory, USGS, NOAA, Aames Research Center JAS Educational Publications 2601 Oakdale Road, H2 P.O. Box 197 Modesto California 95355 1-888-586-6252 Website: http://.Introastro.com Printing by Minuteman Press, Berkley, California ISBN 978-0-9827200-0-4 1 Introduction to Astronomy From Darkness to Blazing Glory The moon Titan is in the forefront with the moon Tethys behind it. These are two of many of Saturn’s moons Credit: Cassini Imaging Team, ISS, JPL, ESA, NASA 2 Introduction to Astronomy Contents in Brief Chapter 1: Astronomy Basics: Pages 1 – 6 Workbook Pages 1 - 2 Chapter 2: Time: Pages 7 - 10 Workbook Pages 3 - 4 Chapter 3: Solar System Overview: Pages 11 - 14 Workbook Pages 5 - 8 Chapter 4: Our Sun: Pages 15 - 20 Workbook Pages 9 - 16 Chapter 5: The Terrestrial Planets: Page 21 - 39 Workbook Pages 17 - 36 Mercury: Pages 22 - 23 Venus: Pages 24 - 25 Earth: Pages 25 - 34 Mars: Pages 34 - 39 Chapter 6: Outer, Dwarf and Exoplanets Pages: 41-54 Workbook Pages 37 - 48 Jupiter: Pages 41 - 42 Saturn: Pages 42 - 44 Uranus: Pages 44 - 45 Neptune: Pages 45 - 46 Dwarf Planets, Plutoids and Exoplanets: Pages 47 -54 3 Chapter 7: The Moons: Pages: 55 - 66 Workbook Pages 49 - 56 Chapter 8: Rocks and Ice: -
Luminous Blue Variables
Review Luminous Blue Variables Kerstin Weis 1* and Dominik J. Bomans 1,2,3 1 Astronomical Institute, Faculty for Physics and Astronomy, Ruhr University Bochum, 44801 Bochum, Germany 2 Department Plasmas with Complex Interactions, Ruhr University Bochum, 44801 Bochum, Germany 3 Ruhr Astroparticle and Plasma Physics (RAPP) Center, 44801 Bochum, Germany Received: 29 October 2019; Accepted: 18 February 2020; Published: 29 February 2020 Abstract: Luminous Blue Variables are massive evolved stars, here we introduce this outstanding class of objects. Described are the specific characteristics, the evolutionary state and what they are connected to other phases and types of massive stars. Our current knowledge of LBVs is limited by the fact that in comparison to other stellar classes and phases only a few “true” LBVs are known. This results from the lack of a unique, fast and always reliable identification scheme for LBVs. It literally takes time to get a true classification of a LBV. In addition the short duration of the LBV phase makes it even harder to catch and identify a star as LBV. We summarize here what is known so far, give an overview of the LBV population and the list of LBV host galaxies. LBV are clearly an important and still not fully understood phase in the live of (very) massive stars, especially due to the large and time variable mass loss during the LBV phase. We like to emphasize again the problem how to clearly identify LBV and that there are more than just one type of LBVs: The giant eruption LBVs or h Car analogs and the S Dor cycle LBVs. -
Supernova 2007Bi Was a Pair-Instability Explosion
Supernova 2007bi was a pair-instability explosion A. Gal-Yam, Benoziyo Center for Astrophysics, Faculty of Physics, The Weizmann Institute of Science, Rehovot 76100, Israel, P. Mazzali, Max-Planck-Institut f¨ur Astrophysik, Karl-Schwarzschild-Str. 1, 85748 Garching, Germany, and Scuola Normale Superiore, Piazza Cavalieri 7, 56127 Pisa, Italy, E. O. Ofek, Department of Astronomy, 105-24, California Institute of Technology, Pasadena, CA 91125, USA, P. E. Nugent, Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720-3411, USA, S. R. Kulkarni, M. M. Kasliwal, R. M. Quimby, Department of Astronomy, 105-24, California Institute of Technology, Pasadena, CA 91125, USA, A. V. Filippenko, S. B. Cenko, R. Chornock, Department of Astronomy, University of California, Berkeley, CA 94720-3411, USA, R. Waldman, The Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel, D. Kasen, Department of Astronomy and Astrophysics, University of California, Santa Cruz, CA 95064, USA, M. Sullivan, Department of Astrophysics, University of Oxford, Keble Road, Oxford OX1 3RH, UK, arXiv:1001.1156v1 [astro-ph.CO] 7 Jan 2010 E. C. Beshore, Department of Planetary Sciences, Lunar and Planetary Laboratory, 1629 E. University Blvd, Tucson AZ 85721, USA, A. J. Drake, Department of Astronomy, 105-24, California Institute of Technology, Pasadena, CA 91125, USA, R. C. Thomas, Luis W. Alvarez Fellow, Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720-3411, USA, J. S. Bloom, D. Poznanski, A. A. Miller, Department of Astronomy, University of California, Berkeley, CA 94720-3411, USA, R. J. Foley, Clay Fellow, Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, J. -
When Neutron Stars Melt, What’S Left Behind Is Spectacular Explosion
Space oddity implodes. The outer layers are cast off in a When neutron stars melt, what’s left behind is spectacular explosion. What’s left behind is truly strange. Anil Ananthaswamy reports a rapidly spinning neutron star, which as the name implies is made mainly of neutrons, with a crust of iron. Whirling up to 1000 times per second, a neutron star is constantly shedding magnetic fields. Over time, this loss of energy causes the star to spin slower and slower. As it spins down, the centrifugal forces that kept gravity at bay start weakening, allowing gravity to squish the star still further. In what is a blink of an eye in cosmic time, the neutrons can be converted to strange N 22 September last year, the website of fundamental building blocks of matter in quark matter, which is a soup of up, down and The Astronomer’s Telegram alerted ways that even machines like the Large strange quarks. In theory, this unusual change Oresearchers to a supernova explosion in Hadron Collider cannot. happens when the density inside the neutron a spiral galaxy about 84 million light years Astrophysicists can thank string theorist star starts increasing. New particles called away. There was just one problem. The same Edward Witten for quark stars. In 1984, he hyperons begin forming that contain at least object, SN 2009ip, had blown up in a similarly hypothesised that protons and neutrons one strange quark bound to others. spectacular fashion just weeks earlier. Such may not be the most stable forms of matter. However, the appearance of hyperons stars shouldn’t go supernova twice, let alone Both are made of two types of smaller marks the beginning of the end of the neutron in quick succession. -
PRODUCT CATALOG Our Journey
2020 PRODUCT CATALOG Our Journey NOVA OPENS 2,500 LAUNCH OF RETAIL CHICAGO DISTRIBUTION SQUARE FT WAREHOUSE BATHROOM SAFETY CENTER OPENS IN EL SEGUNDO, CA PRODUCT LINE 1993 1995 2001 2004 1994 1999 2003 SUE STARTS NOVA THE NOVA BRAKES NOVA EXPANDS WITH AND RON JOINS A NOVA COMES OUT REVAMP AND BECOME LOS ANGELES FEW MONTHS LATER WITH A RED ROLLATOR THE BEST IN CLASS DISTRIBUTION CENTER NOVA THROUGH THE YEARS NOVA Circa 1993 live! LAUNCH OF THE FIRST KICK OFF RETAIL NOVALIVE! LAUNCHED TO ATLANTA DISTRIBUTION SPINNING CANE RACK - REVOLUTION AND LOSE THE TRAIN EVERYONE FROM CENTER OPENS THE CANE CAROUSEL TENNIS BALLS CAMPAIGNS ANYWHERE 2009 2013 2018 2005 2011 2015 2020 NOVA’S LOGO GETS A BIG NOVA’S RETAIL STORE RETAIL MAKEOVERS MAKEOVER IN 5 COLORS PACKAGING GOES GREEN PASS 500 LOCATIONS Contents amazing EDUCATION & MARKETING .................................. 6 wow PLANOGRAMS & DISPLAYS .................................. 10 style CANES ......................................................... 12 independence WALKERS ...................................................... 34 individuality MOBILITY ACCESSORIES .................................... 50 TABLE OF CONTENTS togetherness TRANSPORT CHAIRS & WHEELCHAIRS ................... 57 safety BATHROOM SAFETY .......................................... 68 comfort CUSHIONS ..................................................... 84 sleep PILLOWS & WEDGES ........................................ 99 well-being LIFE AIDS ..................................................... 105 CHOOSEamazing Our Education -
Astrophysics VLT/UVES Spectroscopy of Wray 977, the Hypergiant
UvA-DARE (Digital Academic Repository) VLT/UVES spectroscopy of Wray 977, the hypergiant companion to the X-ray pulsar GX301-2 Kaper, L.; van der Meer, A.; Najarro, F. DOI 10.1051/0004-6361:20065393 Publication date 2006 Document Version Final published version Published in Astronomy & Astrophysics Link to publication Citation for published version (APA): Kaper, L., van der Meer, A., & Najarro, F. (2006). VLT/UVES spectroscopy of Wray 977, the hypergiant companion to the X-ray pulsar GX301-2. Astronomy & Astrophysics, 457(2), 595- 610. https://doi.org/10.1051/0004-6361:20065393 General rights It is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulations If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. UvA-DARE is a service provided by the library of the University of Amsterdam (https://dare.uva.nl) Download date:02 Oct 2021 A&A 457, 595–610 (2006) Astronomy DOI: 10.1051/0004-6361:20065393 & c ESO 2006 Astrophysics VLT/UVES spectroscopy of Wray 977, the hypergiant companion to the X-ray pulsar GX301−2 L. -
Predictions of Variable Mass Loss for Luminous Blue Variables
A&A 393, 543–553 (2002) Astronomy DOI: 10.1051/0004-6361:20021009 & c ESO 2002 Astrophysics Predictions of variable mass loss for Luminous Blue Variables Jorick S. Vink1;2 and A. de Koter3 1 Imperial College, Blackett Laboratory, Prince Consort Road, London, SW7 2BZ, UK 2 Astronomical Institute, Utrecht University, PO Box 80000, 3508 TA Utrecht, The Netherlands 3 Astronomical Institute “Anton Pannekoek”, University of Amsterdam, Kruislaan 403, 1098 SJ Amsterdam, The Netherlands Received 16 April 2002 / Accepted 8 July 2002 Abstract. We present radiation-driven wind models for Luminous Blue Variables (LBVs) and predict their mass-loss rates. We study the effects of lower masses and modified abundances in comparison to the normal OB supergiants, and we find that the main difference in mass loss is due to the lower masses of LBVs. In addition, we find that the increase in helium abundance changes the mass-loss properties by small amounts (up to about 0.2 dex in log M˙ ), while CNO processing is relatively unimportant for the mass-loss rate. A comparison between our mass loss predictions and the observations is performed for four relatively well-studied LBVs. The comparison shows that (i) the winds of LBVs are driven by radiation pressure on spectral lines, (ii) the variable mass loss behaviour of LBVs during their S Doradus-type variation cycles is explained by changes in the line driving efficiency, notably due to the recombination/ionisation of Fe iv/iii and Fe iii/ii, and finally, (iii) the winds of LBVs can be used to derive their masses, as exemplified by the case of AG Car, for which we derive a present-day mass of 35 M . -
Blasts from the Past Historic Supernovas
BLASTS from the PAST: Historic Supernovas 185 386 393 1006 1054 1181 1572 1604 1680 RCW 86 G11.2-0.3 G347.3-0.5 SN 1006 Crab Nebula 3C58 Tycho’s SNR Kepler’s SNR Cassiopeia A Historical Observers: Chinese Historical Observers: Chinese Historical Observers: Chinese Historical Observers: Chinese, Japanese, Historical Observers: Chinese, Japanese, Historical Observers: Chinese, Japanese Historical Observers: European, Chinese, Korean Historical Observers: European, Chinese, Korean Historical Observers: European? Arabic, European Arabic, Native American? Likelihood of Identification: Possible Likelihood of Identification: Probable Likelihood of Identification: Possible Likelihood of Identification: Possible Likelihood of Identification: Definite Likelihood of Identification: Definite Likelihood of Identification: Possible Likelihood of Identification: Definite Likelihood of Identification: Definite Distance Estimate: 8,200 light years Distance Estimate: 16,000 light years Distance Estimate: 3,000 light years Distance Estimate: 10,000 light years Distance Estimate: 7,500 light years Distance Estimate: 13,000 light years Distance Estimate: 10,000 light years Distance Estimate: 7,000 light years Distance Estimate: 6,000 light years Type: Core collapse of massive star Type: Core collapse of massive star Type: Core collapse of massive star? Type: Core collapse of massive star Type: Thermonuclear explosion of white dwarf Type: Thermonuclear explosion of white dwarf? Type: Core collapse of massive star Type: Thermonuclear explosion of white dwarf Type: Core collapse of massive star NASA’s ChANdrA X-rAy ObServAtOry historic supernovas chandra x-ray observatory Every 50 years or so, a star in our Since supernovas are relatively rare events in the Milky historic supernovas that occurred in our galaxy. Eight of the trine of the incorruptibility of the stars, and set the stage for observed around 1671 AD. -
Quark Nova with the Producing of Color-Flavor Locked Quark Matter
Quark Nova with the Producing of Color-Flavor Locked Quark Matter Jia-rui Guo NanKai University, Tianjin 300071, China ∗ September 3, 2021 Abstract In this paper, we suggest that the process in quark nova explosion may exist widely in various kinds of supernova, although it only happens in a small part in the core in most cases. And the contribution to the en- ergy releasing of whole supernova explosion can also be provided by QCD interacting term. In this way we derive a general equation of energy quan- tity to be released in quark nova process related to several parameters. After quark nova explosion process, the remnant can be a quark star, or a neutron star with quark matter core if this process only happens in a small part inside the compact star instead of a \full" quark nova. We will also use a more generalized approach to analyse the strangelets released from quark nova and will draw a possible interpretation of why effects caused by strangelets have not been observed yet. Our result suggests that the ordinary matter can only spontaneously transform into strange quark matter by crushing them into high pressure under the extreme con- dition in compact star, although generally the reaction would really be exergonic. I Introduction Quark nova is a secondary collapsing after neutron stars preliminary formed and it can possibly give a considerable effect to the whole supernova event. It releases energy because the quark matter state is believed to be the ground state of matter [1]. In an environment of high density and high pressure, the quark matter is believed to be in Color-Flavor Locked (CFL) phase in the compact stars [2]. -
The Swirling Hydrogen Gas on the Surface of the Star Rho Gassiopeia Is Turbu at Best; a Seething, Frothing Mass, Normally Radiating at a Temperature of Z,OOO Kelvin
ASTRONOMY N('YY The swirling hydrogen gas on the surface of the star Rho Gassiopeia is turbu at best; a seething, frothing mass, normally radiating at a temperature of Z,OOO Kelvin. Keith Cooper explains what happens when, periodically, Rho Gassiopeia's turbulence gets the better of it. he onset of an eruption is sig- naled when gas begins to swirl and fall in towards the centre of the star.The pressure rises, compressingand heating the gas,causing the starto brightenbriefly.Essentially, the star is coiling up like a spring on a trampo- line and.within months.it bouncesback. In the summer of the year 2000hydro- gen gas measuringten thousandEarth masseswas blastedout from the surface ofRho Cas,the largestsurface eruption ever observed on a star. A shock wave of material now encircles the star that could form aplanetarynebulaearound Rho Cas similar to the Homunculus Nebula around the star Eta Carinae.During the eruption Rho Cas'surface temperature dropped three thousand degreesto a relatively cool4,000It andalreadythe star's surface is recoiling again,perhaps preparing for The constellation of Cassiopeia, home of the hypergiant Rho Cas. lmage: Nik Szymanek. an evenbigger eruption. Welcometo the explosivelife of ahypergiant. ity of these stars,the individual stepson of a solar mass,and in the spaceof ten Rho Casbelongs to a rare breed of stars the path to this void haveyet to be seen. thousandyears it will undergo two hun- known as'hypergiants', of which only Very little is known about the stellar dred eruptions. In total, if each eruption twelve are known to exist in the Galaxy, mechanics involved, or even whether is similar in size,this will accumulateto 'yellow and only sevenare hypergiants' hypergiants can actually reach the Void the equivalent of twenty solar masses like Rho Cas.These stars are extremely before they blow themselvesapart in a ejected from the star. -
Astronomy General Information
ASTRONOMY GENERAL INFORMATION HERTZSPRUNG-RUSSELL (H-R) DIAGRAMS -A scatter graph of stars showing the relationship between the stars’ absolute magnitude or luminosities versus their spectral types or classifications and effective temperatures. -Can be used to measure distance to a star cluster by comparing apparent magnitude of stars with abs. magnitudes of stars with known distances (AKA model stars). Observed group plotted and then overlapped via shift in vertical direction. Difference in magnitude bridge equals distance modulus. Known as Spectroscopic Parallax. SPECTRA HARVARD SPECTRAL CLASSIFICATION (1-D) -Groups stars by surface atmospheric temp. Used in H-R diag. vs. Luminosity/Abs. Mag. Class* Color Descr. Actual Color Mass (M☉) Radius(R☉) Lumin.(L☉) O Blue Blue B Blue-white Deep B-W 2.1-16 1.8-6.6 25-30,000 A White Blue-white 1.4-2.1 1.4-1.8 5-25 F Yellow-white White 1.04-1.4 1.15-1.4 1.5-5 G Yellow Yellowish-W 0.8-1.04 0.96-1.15 0.6-1.5 K Orange Pale Y-O 0.45-0.8 0.7-0.96 0.08-0.6 M Red Lt. Orange-Red 0.08-0.45 *Very weak stars of classes L, T, and Y are not included. -Classes are further divided by Arabic numerals (0-9), and then even further by half subtypes. The lower the number, the hotter (e.g. A0 is hotter than an A7 star) YERKES/MK SPECTRAL CLASSIFICATION (2-D!) -Groups stars based on both temperature and luminosity based on spectral lines.