Calibration Against Spectral Types and VK Color Subm
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Plotting Variable Stars on the H-R Diagram Activity
Pulsating Variable Stars and the Hertzsprung-Russell Diagram The Hertzsprung-Russell (H-R) Diagram: The H-R diagram is an important astronomical tool for understanding how stars evolve over time. Stellar evolution can not be studied by observing individual stars as most changes occur over millions and billions of years. Astrophysicists observe numerous stars at various stages in their evolutionary history to determine their changing properties and probable evolutionary tracks across the H-R diagram. The H-R diagram is a scatter graph of stars. When the absolute magnitude (MV) – intrinsic brightness – of stars is plotted against their surface temperature (stellar classification) the stars are not randomly distributed on the graph but are mostly restricted to a few well-defined regions. The stars within the same regions share a common set of characteristics. As the physical characteristics of a star change over its evolutionary history, its position on the H-R diagram The H-R Diagram changes also – so the H-R diagram can also be thought of as a graphical plot of stellar evolution. From the location of a star on the diagram, its luminosity, spectral type, color, temperature, mass, age, chemical composition and evolutionary history are known. Most stars are classified by surface temperature (spectral type) from hottest to coolest as follows: O B A F G K M. These categories are further subdivided into subclasses from hottest (0) to coolest (9). The hottest B stars are B0 and the coolest are B9, followed by spectral type A0. Each major spectral classification is characterized by its own unique spectra. -
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. -
SHELL BURNING STARS: Red Giants and Red Supergiants
SHELL BURNING STARS: Red Giants and Red Supergiants There is a large variety of stellar models which have a distinct core – envelope structure. While any main sequence star, or any white dwarf, may be well approximated with a single polytropic model, the stars with the core – envelope structure may be approximated with a composite polytrope: one for the core, another for the envelope, with a very large difference in the “K” constants between the two. This is a consequence of a very large difference in the specific entropies between the core and the envelope. The original reason for the difference is due to a jump in chemical composition. For example, the core may have no hydrogen, and mostly helium, while the envelope may be hydrogen rich. As a result, there is a nuclear burning shell at the bottom of the envelope; hydrogen burning shell in our example. The heat generated in the shell is diffusing out with radiation, and keeps the entropy very high throughout the envelope. The core – envelope structure is most pronounced when the core is degenerate, and its specific entropy near zero. It is supported against its own gravity with the non-thermal pressure of degenerate electron gas, while all stellar luminosity, and all entropy for the envelope, are provided by the shell source. A common property of stars with well developed core – envelope structure is not only a very large jump in specific entropy but also a very large difference in pressure between the center, Pc, the shell, Psh, and the photosphere, Pph. Of course, the two characteristics are closely related to each other. -
Temperature, Mass and Size of Stars
Title Astro100 Lecture 13, March 25 Temperature, Mass and Size of Stars http://www.astro.umass.edu/~myun/teaching/a100/longlecture13.html Also, http://www.astro.columbia.edu/~archung/labs/spring2002/spring2002.html (Lab 1, 2, 3) Goal Goal: To learn how to measure various properties of stars 9 What properties of stars can astronomers learn from stellar spectra? Î Chemical composition, surface temperature 9 How useful are binary stars for astronomers? Î Mass 9 What is Stefan-Boltzmann Law? Î Luminosity, size, temperature 9 What is the Hertzsprung-Russell Diagram? Î Distance and Age Temp1 Stellar Spectra Spectrum: light separated and spread out by wavelength using a prism or a grating BUT! Stellar spectra are not continuous… Temp2 Stellar Spectra Photons from inside of higher temperature get absorbed by the cool stellar atmosphere, resulting in “absorption lines” At which wavelengths we see these lines depends on the chemical composition and physical state of the gas Temp3 Stellar Spectra Using the most prominent absorption line (hydrogen), Temp4 Stellar Spectra Measuring the intensities at different wavelength, Intensity Wavelength Wien’s Law: λpeak= 2900/T(K) µm The hotter the blackbody the more energy emitted per unit area at all wavelengths. The peak emission from the blackbody moves to shorter wavelengths as the T increases (Wien's law). Temp5 Stellar Spectra Re-ordering the stellar spectra with the temperature Temp-summary Stellar Spectra From stellar spectra… Surface temperature (Wien’s Law), also chemical composition in the stellar -
The Spitzer Space Telescope First-Look Survey. II. KPNO
The Spitzer Space Telescope First-Look Survey: KPNO MOSAIC-1 R-band Images and Source Catalogs Dario Fadda1, Buell T. Jannuzi2, Alyson Ford2, Lisa J. Storrie-Lombardi1 [January, 2004 { Submitted to AJ] ABSTRACT We present R-band images covering more than 11 square degrees of sky that were obtained in preparation for the Spitzer Space Telescope First Look Survey (FLS). The FLS was designed to characterize the mid-infrared sky at depths 2 orders of magnitude deeper than previous surveys. The extragalactic component is the ¯rst cosmological survey done with Spitzer. Source catalogs extracted from the R-band images are also presented. The R-band images were obtained using the MOSAIC-1 camera on the Mayall 4m telescope of the Kitt Peak National Observatory. Two relatively large regions of the sky were observed to modest depth: the main FLS extra galac- tic ¯eld (17h18m00s +59o3000000:0 J2000; l= 88:3, b= +34:9) and ELAIS-N1 ¯eld (16h10m01s +54o3003600:0 J2000; l= 84:2, b= +44:9). While both of these ¯elds were in early plans for the FLS, only a single deep pointing test observation were made at the ELAIS-N1 location. The larger Legacy program SWIRE (Lonsdale et al., 2003) will include this region among its sur- veyed areas. The data products of our KPNO imaging (images and object catalogs) are made available to the community through the World Wide Web (via the Spitzer Science Center and NOAO Science Archives). The overall quality of the images is high. The measured positions of sources detected in the images have RMS uncertainties in their absolute positions of order 0.35 arc-seconds with possible systematic o®sets of order 0.1 arc-seconds, depending on the reference frame of comparison. -
Publications of the Astronomical Society of the Pacific 97:165-174, Febmary 1985
Publications of the Astronomical Society of the Pacific 97:165-174, Febmary 1985 PHOTOMETRY OF STARS IN THE uvgr SYSTEM* STEPHEN M. KENT Harvard-Smithsonian Center for Astrophysics, 60 Garden Street Cambridge, Massachusetts 02138 Received 1984 July 23, revised 1984 November 17 Photoelectric photometry is presented for over 400 stars using the uvgr system of Thuan and Gunn. Stars were selected to cover a wide range of spectral type, luminosity class, and metallicity. A mean main sequence is derived along with red- dening curves and approximate transformations to the UBVR system. The calibration of the standard-star sequence is sig- nificantly improved. Key words: photometry—stellar classification I. Introduction II. Observations The uvgr system (Thuan and Gunn 1976, hereafter The observations were made during several runs from TG) was developed as a four-color intermediate-to-wide- 1976 through 1978 on the Palomar 60-inch (1.5-m) tele- band photometric system which was designed to avoid a scope. The instrumentation and equipment were identi- number of pitfalls of the standard UBV system. The four cal with that used by TG. A two-channel pulse-counting bands are nonoverlapping and exclude the strongest S20 photometer allowed for the simultaneous measure- night-sky lines. The u and ν filters lie in a region of ment of object and sky. Each star was observed in both strong line blanketing in late-type stars and measure the apertures except for the globular-cluster stars, where it Balmer jump in early-type stars; the g and r filters lie in was necessary to go off the cluster to measure sky. -
Mass-Radius Relations for Massive White Dwarf Stars
A&A 441, 689–694 (2005) Astronomy DOI: 10.1051/0004-6361:20052996 & c ESO 2005 Astrophysics Mass-radius relations for massive white dwarf stars L. G. Althaus1,, E. García-Berro1,2, J. Isern2,3, and A. H. Córsico4,5, 1 Departament de Física Aplicada, Universitat Politècnica de Catalunya, Av. del Canal Olímpic, s/n, 08860 Castelldefels, Spain e-mail: [leandro;garcia]@fa.upc.es 2 Institut d’Estudis Espacials de Catalunya, Ed. Nexus, c/Gran Capità 2, 08034 Barcelona, Spain e-mail: [email protected] 3 Institut de Ciències de l’Espai, C.S.I.C., Campus UAB, Facultat de Ciències, Torre C-5, 08193 Bellaterra, Spain 4 Facultad de Ciencias Astronómicas y Geofísicas, Universidad Nacional de La Plata, Paseo del Bosque s/n, (1900) La Plata, Argentina e-mail: [email protected] 5 Instituto de Astrofísica La Plata, IALP, CONICET, Argentina Received 4 March 2005 / Accepted 18 July 2005 Abstract. We present detailed theoretical mass-radius relations for massive white dwarf stars with oxygen-neon cores. This work is motivated by recent observational evidence about the existence of white dwarf stars with very high surface gravities. Our results are based on evolutionary calculations that take into account the chemical composition expected from the evolu- tionary history of massive white dwarf progenitors. We present theoretical mass-radius relations for stellar mass values ranging from1.06to1.30 M with a step of 0.02 M and effective temperatures from 150 000 K to ≈5000 K. A novel aspect predicted by our calculations is that the mass-radius relation for the most massive white dwarfs exhibits a marked dependence on the neutrino luminosity. -
Part V Stellar Spectroscopy
Part V Stellar spectroscopy 53 Chapter 10 Classification of stellar spectra Goal-of-the-Day To classify a sample of stars using a number of temperature-sensitive spectral lines. 10.1 The concept of spectral classification Early in the 19th century, the German physicist Joseph von Fraunhofer observed the solar spectrum and realised that there was a clear pattern of absorption lines superimposed on the continuum. By the end of that century, astronomers were able to examine the spectra of stars in large numbers and realised that stars could be divided into groups according to the general appearance of their spectra. Classification schemes were developed that grouped together stars depending on the prominence of particular spectral lines: hydrogen lines, helium lines and lines of some metallic ions. Astronomers at Harvard Observatory further developed and refined these early classification schemes and spectral types were defined to reflect a smooth change in the strength of representative spectral lines. The order of the spectral classes became O, B, A, F, G, K, and M; even though these letter designations no longer have specific meaning the names are still in use today. Each spectral class is divided into ten sub-classes, so that for instance a B0 star follows an O9 star. This classification scheme was based simply on the appearance of the spectra and the physical reason underlying these properties was not understood until the 1930s. Even though there are some genuine differences in chemical composition between stars, the main property that determines the observed spectrum of a star is its effective temperature. -
Download the AAS 2011 Annual Report
2011 ANNUAL REPORT AMERICAN ASTRONOMICAL SOCIETY aas mission and vision statement The mission of the American Astronomical Society is to enhance and share humanity’s scientific understanding of the universe. 1. The Society, through its publications, disseminates and archives the results of astronomical research. The Society also communicates and explains our understanding of the universe to the public. 2. The Society facilitates and strengthens the interactions among members through professional meetings and other means. The Society supports member divisions representing specialized research and astronomical interests. 3. The Society represents the goals of its community of members to the nation and the world. The Society also works with other scientific and educational societies to promote the advancement of science. 4. The Society, through its members, trains, mentors and supports the next generation of astronomers. The Society supports and promotes increased participation of historically underrepresented groups in astronomy. A 5. The Society assists its members to develop their skills in the fields of education and public outreach at all levels. The Society promotes broad interest in astronomy, which enhances science literacy and leads many to careers in science and engineering. Adopted 7 June 2009 A S 2011 ANNUAL REPORT - CONTENTS 4 president’s message 5 executive officer’s message 6 financial report 8 press & media 9 education & outreach 10 membership 12 charitable donors 14 AAS/division meetings 15 divisions, committees & workingA groups 16 publishing 17 public policy A18 prize winners 19 member deaths 19 society highlights Established in 1899, the American Astronomical Society (AAS) is the major organization of professional astronomers in North America. -
Arxiv:2106.01477V1 [Astro-Ph.IM] 2 Jun 2021 Document in Their Instructions to Authors
Draft version June 4, 2021 Typeset using LATEX twocolumn style in AASTeX63 Best Practices for Data Publication in the Astronomical Literature Tracy X. Chen,1 Marion Schmitz,1 Joseph M. Mazzarella,1 Xiuqin Wu,1 Julian C. van Eyken,2 Alberto Accomazzi,3 Rachel L. Akeson,2 Mark Allen,4 Rachael Beaton,5 G. Bruce Berriman,2 Andrew W. Boyle,2 Marianne Brouty,4 Ben Chan,1 Jessie L. Christiansen,2 David R. Ciardi,2 David Cook,1 Raffaele D'Abrusco,3 Rick Ebert,1 Cren Frayer,1 Benjamin J. Fulton,2 Christopher Gelino,2 George Helou,1 Calen B. Henderson,2 Justin Howell,6 Joyce Kim,1 Gilles Landais,4 Tak Lo,1 Cecile Loup,4 Barry Madore,7, 8 Giacomo Monari,4 August Muench,9 Anais Oberto,4 Pierre Ocvirk,4 Joshua E. G. Peek,10, 11 Emmanuelle Perret,4 Olga Pevunova,1 Solange V. Ramirez,7 Luisa Rebull,6 Ohad Shemmer,12 Alan Smale,13 Raymond Tam,2 Scott Terek,1 Doug Van Orsow,13, 14 Patricia Vannier,4 and Shin-Ywan Wang1 1Caltech/IPAC-NED, Mail Code 100-22, Caltech, 1200 E. California Blvd., Pasadena, CA 91125, USA 2Caltech/IPAC-NExScI, Mail Code 100-22, Caltech, 1200 E. California Blvd., Pasadena, CA 91125, USA 3Center for Astrophysics j Harvard & Smithsonian, 60 Garden Street, Cambridge, MA 02138, USA 4Centre de Donn´eesastronomiques de Strasbourg, Observatoire de Strasbourg, 11, rue de l'Universit´e,67000 STRASBOURG, France 5Department of Astrophysical Sciences, Princeton University, 4 Ivy Lane, Princeton, NJ 08544, USA 6Caltech/IPAC-IRSA, Mail Code 100-22, Caltech, 1200 E. -
White Dwarfs - Degenerate Stellar Configurations
White Dwarfs - Degenerate Stellar Configurations Austen Groener Department of Physics - Drexel University, Philadelphia, Pennsylvania 19104, USA Quantum Mechanics II May 17, 2010 Abstract The end product of low-medium mass stars is the degenerate stellar configuration called a white dwarf. Here we discuss the transition into this state thermodynamically as well as developing some intuition regarding the role of quantum mechanics in this process. I Introduction and Stellar Classification present at such high temperatures are small com- pared with the kinetic (thermal) energy of the parti- It is widely believed that the end stage of the low or cles. This assumption implies a mixture of free non- intermediate mass star is an extremely dense, highly interacting particles. One may also note that the pres- underluminous object called a white dwarf. Obser- sure of a mixture of different species of particles will vationally, these white dwarfs are abundant (∼ 6%) be the sum of the pressures exerted by each (this is in the Milky Way due to a large birthrate of their pro- where photon pressure (PRad) will come into play). genitor stars coupled with a very slow rate of cooling. Following this logic we can express the total stellar Roughly 97% of all stars will meet this fate. Given pressure as: no additional mass, the white dwarf will evolve into a cold black dwarf. PT ot = PGas + PRad = PIon + Pe− + PRad (1) In this paper I hope to introduce a qualitative de- scription of the transition from a main-sequence star At Hydrostatic Equilibrium: Pressure Gradient = (classification which aligns hydrogen fusing stars Gravitational Pressure. -
Redox DAS Artist List for Period: 01.09.2017
Page: 1 Redox D.A.S. Artist List for period: 01.09.2017 - 30.09.2017 Date time: Number: Title: Artist: Publisher Lang: 01.09.2017 00:00:40 HD 15073 NOCOJ LJUBILA BI SE S TEBOJ DAMJANA GOLAVSEK IN HOT HOT HOT SLO 01.09.2017 00:04:10 HD 31975 GOOD OLE BOYS LIKE ME DON WILLIAMS ANG 01.09.2017 00:08:22 HD 25035 YEARS GUNS N' ROSES ANG 01.09.2017 00:12:37 HD 44397 VEDNO ME LAHKO POKLICES NINA OSENAR SLO 01.09.2017 00:16:26 HD 38796 CAN & CANNOT DO GIA FARRELL ANG 01.09.2017 00:20:19 HD 03104 BLACK COFFEE ALL SAINTS ANG 01.09.2017 00:24:57 HD 13851 NAJ TI BO LEPO PIRAMIDA SLO 01.09.2017 00:28:40 HD 52192 THE CONVERSATION TEXAS ANG 01.09.2017 00:31:33 HD 05827 GOOD TIMES POINTER SISTERS ANG 01.09.2017 00:35:09 HD 12363 NE IZZIVAJ ME DON MENTONY BAND SLO 01.09.2017 00:39:43 HD 07165 NEVER LEAVE YOU (RMX) LUMIDEE FEAT. BUSTA RHYMES ANG 01.09.2017 00:43:23 HD 54905 LIMBO DADDY YANKEE SPA 01.09.2017 00:47:08 HD 52264 KO BOM UMRL FLIRRT SLO 01.09.2017 00:50:15 HD 58268 SUMMER STORY ZAN SERCIC SLO 01.09.2017 00:53:21 HD 45692 SUMMER DAY SHERYL CROW ANG 01.09.2017 00:57:11 HD 52251 ZAPLEZALI SMO SE ZORAN PREDIN IN COVERLOVER SLO 01.09.2017 01:00:44 HD 05897 THE SHOW MUST GO ON QUEEN ANG 01.09.2017 01:04:58 HD 58371 LAY YOU DOWN EASY MAGIC FEAT SEAN PAUL ANG 01.09.2017 01:07:40 HD 55050 RIBICA MARKO VOZELJ & MOJS3 SLO 01.09.2017 01:11:06 HD 55085 PRAYER IN C LILLY WOOD & THE PRICK AND ROBIN SCHULZ ANG 01.09.2017 01:14:26 HD 25011 PARADISE CITY GUNS N' ROSES ANG 01.09.2017 01:21:11 HD 52218 LJUBEZEN NA DALJAVO FELIKS LANGUS SLO 01.09.2017 01:23:49 HD 55951 I NEED YOUR LOVE (FEAT.