The Different Origins of Magnetic Fields and Activity in the Hertzsprung Gap
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Hertzsprung-Russell Diagram and Mass Distribution of Barium Stars ? A
Astronomy & Astrophysics manuscript no. HRD_Ba c ESO 2019 May 14, 2019 Hertzsprung-Russell diagram and mass distribution of barium stars ? A. Escorza1; 2, H.M.J. Boffin3, A.Jorissen2, S. Van Eck2, L. Siess2, H. Van Winckel1, D. Karinkuzhi2, S. Shetye2; 1, and D. Pourbaix2 1 Institute of Astronomy, KU Leuven, Celestijnenlaan 200D, 3001 Leuven, Belgium 2 Institut d’Astronomie et d’Astrophysique, Université Libre de Bruxelles, ULB, Campus Plaine C.P. 226, Boulevard du Triomphe, B-1050 Bruxelles, Belgium 3 ESO, Karl Schwarzschild Straße 2, D-85748 Garching bei München, Germany Received; Accepted ABSTRACT With the availability of parallaxes provided by the Tycho-Gaia Astrometric Solution, it is possible to construct the Hertzsprung-Russell diagram (HRD) of barium and related stars with unprecedented accuracy. A direct result from the derived HRD is that subgiant CH stars occupy the same region as barium dwarfs, contrary to what their designations imply. By comparing the position of barium stars in the HRD with STAREVOL evolutionary tracks, it is possible to evaluate their masses, provided the metallicity is known. We used an average metallicity [Fe/H] = −0.25 and derived the mass distribution of barium giants. The distribution peaks around 2.5 M with a tail at higher masses up to 4.5 M . This peak is also seen in the mass distribution of a sample of normal K and M giants used for comparison and is associated with stars located in the red clump. When we compare these mass distributions, we see a deficit of low-mass (1 – 2 M ) barium giants. -
Module 14 H. R. Diagram TABLE of CONTENTS 1. Learning Outcomes
Module 14 H. R. Diagram TABLE OF CONTENTS 1. Learning Outcomes 2. Introduction 3. H. R. Diagram 3.1. Coordinates of H. R. Diagram 3.2. Stellar Families 3.3. Hertzsprung Gap 3.4. H. R. Diagram and Stellar Radii 4. Summary 1. Learning Outcomes After studying this module, you should be able to recognize an H. R. Diagram explain the coordinates of an H. R. Diagram appreciate the shape of an H. R. Diagram understand that in this diagram stars appear in distinct families recount the characteristics of these families recognize that there is a real gap in the horizontal branch of the diagram, called the Hertzsprung gap explain that during their evolution stars pass very rapidly through this region and therefore there is a real paucity of stars here derive the shape of the 퐥퐨퐠 푻 − 퐥퐨퐠 푳 plot at a given stellar radius explain that the stellar radius (and mass) increases upwards in the H. R. Diagram 2. Introduction In the last few modules we have discussed the stellar spectra and spectral classification based on stellar spectra. The Harvard system of spectral classification categorized stellar spectra in 7 major classes, from simple spectra containing only a few lines to spectra containing a huge number of lines and molecular bands. The major classes were named O, B, A, F, G, K and M. Each major class was further subdivided into 10 subclasses, running from 0 to 9. Considering the bewildering variety of stellar spectra, classes Q, P and Wolf-Rayet had to be introduced at the top of the classification and classes R and N were introduced at the bottom of the classification scheme. -
Structure and Evolution of FK Comae Corona
A&A 383, 919–932 (2002) Astronomy DOI: 10.1051/0004-6361:20011810 & c ESO 2002 Astrophysics Structure and evolution of FK Comae corona P. Gondoin, C. Erd, and D. Lumb Space Science Department, European Space Agency – Postbus 299, 2200 AG Noordwijk, The Netherlands Received 16 October 2001 / Accepted 17 December 2001 Abstract. FK Comae (HD 117555) is a rapidly rotating single G giant whose distinctive characteristics include a quasisinusoidal optical light curve and high X-ray luminosity. FK Comae was observed twice at two weeks interval in January 2001 by the XMM-Newton space observatory. Analysis results suggest a scenario where the corona of FK Comae is dominated by large magnetic structures similar in size to interconnecting loops between solar active regions but significantly hotter. The interaction of these structures themselves could explain the permanent flaring activity on large scales that is responsible for heating FK Comae plasma to high temperatures. During our observations, these flares were not randomly distributed on the star surface but were partly grouped within a large compact region of about 30 degree extent in longitude reminiscent of a large photospheric spot. We argue that the α − Ω dynamo driven activity on FK Comae will disappear in the future with the effect of suppressing large scale magnetic structures in its corona. Key words. stars: individual: FK Comae – stars: activity – stars: coronae – stars: evolution – stars: late-type – X-ray: stars 1. Introduction ments and their temporal behaviour during the observa- tions. Sections 5 and 6 describe the spectral analysis of the FK Comae (HD 117555) is the prototype of a small group EPIC and RGS datasets. -
Post-Main Sequence Evolution – Low and Intermediate Mass Stars
Post-Main Sequence Evolution – Low and Intermediate Mass Stars Pols 10, 11 Prialnik 9 Glatzmaier and Krumholz 16 • Once hydrogen is exhausted in the inner part of the star, it is no longer a main What happens when sequence star. It continues to burn the sun runs out of hydrogen in a thick shell around the helium hydrogen in its center? core, and actually grows more luminous. • Once the SC mass is exceeded, the contraction of the H-depleted core takes the hydrogen burning shell to H greater depth and higher temperature. He it burns very vigorously with a luminosity set more by the properties of the helium core than the unburned “envelope” of the star. The shell becomes thin in response to a reduced pressure scale height at the core’s edge because of its high gravity. L • The evolution differs for stars below about 2 solar masses and above. The helium core becomes degenerate as T ← it contracts for the lower mass stars • H shell burning is by the CNO cycle and What happens when therefore very temperature sensitive. the sun runs out of hydrogen in its center? • In stars lighter than the sun where a large fraction of the outer mass was already convective on the main sequence, the increased luminosity is transported quickly to the surface and the stars luminosity rises at nearly H constant photospheric temperature He (i.e., the star is already on the Hayashi strip) • For more massive stars, the surface remains radiative for a time and the luminosity continues to be set by the L mass of the star (i.e., is constant). -
Hertzsprung-Russell Diagram and Mass Distribution of Barium Stars? A
A&A 608, A100 (2017) Astronomy DOI: 10.1051/0004-6361/201731832 & c ESO 2017 Astrophysics Hertzsprung-Russell diagram and mass distribution of barium stars? A. Escorza1; 2, H. M. J. Boffin3, A. Jorissen2, S. Van Eck2, L. Siess2, H. Van Winckel1, D. Karinkuzhi2, S. Shetye2; 1, and D. Pourbaix2 1 Institute of Astronomy, KU Leuven, Celestijnenlaan 200D, 3001 Leuven, Belgium e-mail: [email protected] 2 Institut d’Astronomie et d’Astrophysique, Université Libre de Bruxelles, ULB, Campus Plaine C.P. 226, Boulevard du Triomphe, 1050 Bruxelles, Belgium 3 ESO, Karl Schwarzschild Straße 2, 85748 Garching bei München, Germany Received 25 August 2017 / Accepted 25 September 2017 ABSTRACT With the availability of parallaxes provided by the Tycho-Gaia Astrometric Solution, it is possible to construct the Hertzsprung-Russell diagram (HRD) of barium and related stars with unprecedented accuracy. A direct result from the derived HRD is that subgiant CH stars occupy the same region as barium dwarfs, contrary to what their designations imply. By comparing the position of barium stars in the HRD with STAREVOL evolutionary tracks, it is possible to evaluate their masses, provided the metallicity is known. We used an average metallicity [Fe/H] = −0.25 and derived the mass distribution of barium giants. The distribution peaks around 2.5 M with a tail at higher masses up to 4.5 M . This peak is also seen in the mass distribution of a sample of normal K and M giants used for comparison and is associated with stars located in the red clump. When we compare these mass distributions, we see a deficit of low-mass (1 – 2 M ) barium giants. -
Origin of Spin-Orbit Misalignments: the Microblazar V4641 Sgr
Draft version June 29, 2020 Typeset using LATEX twocolumn style in AASTeX62 Origin of Spin-Orbit Misalignments: The Microblazar V4641 Sgr Greg Salvesen1, 2, 3, ∗ and Supavit Pokawanvit3 1CCS-2, Los Alamos National Laboratory, P.O. Box 1663, Los Alamos, NM 87545, USA. 2Center for Theoretical Astrophysics, Los Alamos National Laboratory, Los Alamos, NM 87545, USA. 3Department of Physics, University of California, Santa Barbara, CA 93106, USA. (Received November 05, 2019; Accepted April 22, 2020; Published June 2020) Submitted to Monthly Notices of the Royal Astronomical Society ABSTRACT Of the known microquasars, V4641 Sgr boasts the most severe lower limit (> 52◦) on the misalign- ment angle between the relativistic jet axis and the binary orbital angular momentum. Assuming the jet and black hole spin axes coincide, we attempt to explain the origin of this extreme spin-orbit misalignment with a natal kick model, whereby an aligned binary system becomes misaligned by a supernova kick imparted to the newborn black hole. The model inputs are the kick velocity distri- bution, which we measure customized to V4641 Sgr, and the immediate pre/post-supernova binary system parameters. Using a grid of binary stellar evolution models, we determine post-supernova configurations that evolve to become consistent with V4641 Sgr today and obtain the corresponding pre-supernova configurations by using standard prescriptions for common envelope evolution. Using each of these potential progenitor system parameter sets as inputs, we find that a natal kick strug- gles to explain the origin of the V4641 Sgr spin-orbit misalignment. Consequently, we conclude that evolutionary pathways involving a standard common envelope phase followed by a supernova kick are highly unlikely for V4641 Sgr. -
This Online Essay Is an Extended Version of the Essay in the Printed-Edition Handbook, Containing All the Material of Its Print
This online essay is an extended version of the essay in the printed-edition Handbook, containing all the material of its printed- edition accompaniment, but adding material of its own. The accompanying online table is likewise an extended version of the printed-edition table, (a) with extra stars (the brightest 313, allowing for variability, where the printed edition has almost 30 fewer, allowing for variability), and (b) with additional remarks for most of the duplicated stars. The online essay and table try to address the needs of three kinds of serious amateur: amateurs who are also astrophysics students (whether or not enrolled formally at some campus); amateurs who, like many in RASC, assist in public outreach, through some form of lecturing; and amateurs who are planning their own private citizen-science observing runs, in the spirit of such “pro-am” organizations as AAVSO. Our online project, now a couple of years old, must be considered still in its early stages. We cannot claim to have fully satisfied the needs of our three constituencies. Above all, we cannot claim to have covered all the appropriate points from stellar- astronomy news in our “Remarks” column, important though news is to amateurs of all three types. We would hope in coming years to remedy our deficiencies in several ways, above all by relying more in our writing on recent primary-literature journal articles, and by making appropriate citations of the primary literature. Already at this early stage, we have tried to pick out a few tens of the more important recent journal articles. -
Stars, Galaxies, and Beyond, 2012
Stars, Galaxies, and Beyond Summary of notes and materials related to University of Washington astronomy courses: ASTR 322 The Contents of Our Galaxy (Winter 2012, Professor Paula Szkody=PXS) & ASTR 323 Extragalactic Astronomy And Cosmology (Spring 2012, Professor Željko Ivezić=ZXI). Summary by Michael C. McGoodwin=MCM. Content last updated 6/29/2012 Rotated image of the Whirlpool Galaxy M51 (NGC 5194)1 from Hubble Space Telescope HST, with Companion Galaxy NGC 5195 (upper left), located in constellation Canes Venatici, January 2005. Galaxy is at 9.6 Megaparsec (Mpc)= 31.3x106 ly, width 9.6 arcmin, area ~27 square kiloparsecs (kpc2) 1 NGC = New General Catalog, http://en.wikipedia.org/wiki/New_General_Catalogue 2 http://hubblesite.org/newscenter/archive/releases/2005/12/image/a/ Page 1 of 249 Astrophysics_ASTR322_323_MCM_2012.docx 29 Jun 2012 Table of Contents Introduction ..................................................................................................................................................................... 3 Useful Symbols, Abbreviations and Web Links .................................................................................................................. 4 Basic Physical Quantities for the Sun and the Earth ........................................................................................................ 6 Basic Astronomical Terms, Concepts, and Tools (Chapter 1) ............................................................................................. 9 Distance Measures ...................................................................................................................................................... -
Post Main Sequence Evolution
Post Main Sequence evolution Contents 1 Introduction1 2 Main sequence evolution and lifetime2 2.1 Main sequence duration..............................2 2.2 Evolution along the main sequence........................3 3 Evolutionary tracks and isochrones5 4 Red giant phase5 4.1 The turn-off point.................................5 4.2 From H burning to He burning: overview....................6 4.3 Giant stars: red or blue..............................7 4.4 Hydrogen shell burning and helium core growth.................7 4.5 The Schonberg-Chandrasekhar¨ limit and the Hertzprung gap..........9 4.6 Low-mass stars: degenerate core and the Helium flash.............. 10 4.7 Horizontal branch: low-mass. core helium burning, stars............ 10 4.8 Sub Giant Branch................................. 10 4.9.......................................... 11 5 Cepheids 11 6 The Asymptotic Giant Branch 11 1 Introduction The density of stars in the HR diagram (or simply HRD) directly tells us where stars spend significant amounts of time. After the main sequence, which is the densest part of the HRD, high density of points in the HRD are found in regions above the MS, namely where the radius is increased. These stars are in the giant region which, as we will see, can be divived into the red giant branch (RGB), the horizontal branch (HB), and the asymptotic giant branch (AGB). The evolution of stars beyond the main sequence is much more complex than that on the main sequence, essentially because the timescale separation not always applies. Nevertheless, some of the basic features of the evolutionary path in the HRD can still be understood using 2 4 simple equations, one of the most useful being L = 4πR σTeff .