Spectral Classification; Old and Contemporary
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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. -
JESUITS, ROLE in GEOMAGNETISM That the Earth Does Not Rotate Because of Its Magnetic Field
Comp. by: DShiva Date:14/2/07 Time:15:55:17 Stage:First Proof File Path://spiina1001z/womat/production/ PRODENV/0000000005/0000001725/0000000022/000000A293.3D Proof by: QC by: J in which, in order to defend the geocentric system, he tried to show JESUITS, ROLE IN GEOMAGNETISM that the Earth does not rotate because of its magnetic field. Among the best observations made in China are those of Antoine Gaubil The Jesuits are members of a religious order of the Catholic Church, (1689–1759), who mentioned that the line of zero declination has with the Society of Jesus, founded in 1540 by Ignatius of Loyola. From time a movement from east to west. His observations and those of 1548, when Jesuits established their first college, their educational other Jesuits in China were published in France in three volumes work expanded rapidly and in the 18th century, in Europe alone, there between 1729 and 1732. In 1727, Nicolas Sarrabat (1698–1739) pub- were 645 colleges and universities and others in Asia and America. As lished Nouvelle hypothèse sur les variations de l’aiguille aimantée, an innovation in these colleges, special attention was given to teaching which was given an award by the Académie des Sciences of Paris. of mathematics, astronomy, and the natural sciences. This tradition has In 1769, Maximilian Hell (1720–1792), director of the observatory been continued in modern times in the many Jesuit colleges and uni- in Vienna, made observations of the magnetic declination during his versities and this tradition thus spread throughout the world. Jesuits’ journey to the island of Vardö in Lapland, at a latitude of 70 N, where interest in geomagnetism derived from teaching in these colleges he observed the transit of Venus over the solar disk. -
P. Angelo Segghi, S. J. 1818 - 18?8
P. ANGELO SEGGHI, S. J. 1818 - 18?8 H. A. BRUCK Pontifical Academician At this commemorative Colloquium which is devoted to "Spectral Classification of the Future" it is fitting that we should speak about the life and work of the man with whom all modern spectral classification started, Father Angelo Secchi who died here in Rome a hundred years ago in February I878. At the time of his death the name of Secchi was renowned throughout the scientific world, and his early death in his 60th year came as a great shock to the whole astronomical com munity - in the same way in which the untimely death of Father Treanor in February of this year is being deplored by astronomers all over the world. Father Secchi was one of the great pioneers of astro physics, or "physical astronomy" as he used to call it, whose work ranged over the widest possible field. He made fundamental contributions to solar physics as well as to stellar spectro scopy and he also worked with considerable success in geophysics and meterology. For 28 years of his life Father Secchi was in charge of the Observatory of the Collegio Romano, the Roman College of the Society of Jesus, an observatory which he transformed into one of the world's best known and most respected scientific establishments. Secchi was an indefatigable worker. In spite of many distracting duties which were forced on him by his official position Secchi managed to publish in the course of his life some seven hundred publications in many of the leading scien tific periodicals of his time in France, Britain, Germany as well as Italy. -
HI Balmer Jump Temperatures for Extragalactic HII Regions in the CHAOS Galaxies
HI Balmer Jump Temperatures for Extragalactic HII Regions in the CHAOS Galaxies A Senior Thesis Presented in Partial Fulfillment of the Requirements for Graduation with Research Distinction in Astronomy in the Undergraduate Colleges of The Ohio State University By Ness Mayker The Ohio State University April 2019 Project Advisors: Danielle A. Berg, Richard W. Pogge Table of Contents Chapter 1: Introduction ............................... 3 1.1 Measuring Nebular Abundances . 8 1.2 The Balmer Continuum . 13 Chapter 2: Balmer Jump Temperature in the CHAOS galaxies .... 16 2.1 Data . 16 2.1.1 The CHAOS Survey . 16 2.1.2 CHAOS Balmer Jump Sample . 17 2.2 Balmer Jump Temperature Determinations . 20 2.2.1 Balmer Continuum Significance . 20 2.2.2 Balmer Continuum Measurements . 21 + 2.2.3 Te(H ) Calculations . 23 2.2.4 Photoionization Models . 24 2.3 Results . 26 2.3.1 Te Te Relationships . 26 − 2.3.2 Discussion . 28 Chapter 3: Conclusions and Future Work ................... 32 1 Abstract By understanding the observed proportions of the elements found across galaxies astronomers can learn about the evolution of life and the universe. Historically, there have been consistent discrepancies found between the two main methods used to measure gas-phase elemental abundances: collisionally excited lines and optical recombination lines in H II regions (ionized nebulae around young star-forming regions). The origin of the discrepancy is thought to hinge primarily on the strong temperature dependence of the collisionally excited emission lines of metal ions, principally Oxygen, Nitrogen, and Sulfur. This problem is exacerbated by the difficulty of measuring ionic temperatures from these species. -
The Formation of Brown Dwarfs 459
Whitworth et al.: The Formation of Brown Dwarfs 459 The Formation of Brown Dwarfs: Theory Anthony Whitworth Cardiff University Matthew R. Bate University of Exeter Åke Nordlund University of Copenhagen Bo Reipurth University of Hawaii Hans Zinnecker Astrophysikalisches Institut, Potsdam We review five mechanisms for forming brown dwarfs: (1) turbulent fragmentation of molec- ular clouds, producing very-low-mass prestellar cores by shock compression; (2) collapse and fragmentation of more massive prestellar cores; (3) disk fragmentation; (4) premature ejection of protostellar embryos from their natal cores; and (5) photoerosion of pre-existing cores over- run by HII regions. These mechanisms are not mutually exclusive. Their relative importance probably depends on environment, and should be judged by their ability to reproduce the brown dwarf IMF, the distribution and kinematics of newly formed brown dwarfs, the binary statis- tics of brown dwarfs, the ability of brown dwarfs to retain disks, and hence their ability to sustain accretion and outflows. This will require more sophisticated numerical modeling than is presently possible, in particular more realistic initial conditions and more realistic treatments of radiation transport, angular momentum transport, and magnetic fields. We discuss the mini- mum mass for brown dwarfs, and how brown dwarfs should be distinguished from planets. 1. INTRODUCTION form a smooth continuum with those of low-mass H-burn- ing stars. Understanding how brown dwarfs form is there- The existence of brown dwarfs was first proposed on the- fore the key to understanding what determines the minimum oretical grounds by Kumar (1963) and Hayashi and Nakano mass for star formation. In section 3 we review the basic (1963). -
Spectroscopy and the Stars
SPECTROSCOPY AND THE STARS K H h g G d F b E D C B 400 nm 500 nm 600 nm 700 nm by DR. STEPHEN THOMPSON MR. JOE STALEY The contents of this module were developed under grant award # P116B-001338 from the Fund for the Improve- ment of Postsecondary Education (FIPSE), United States Department of Education. However, those contents do not necessarily represent the policy of FIPSE and the Department of Education, and you should not assume endorsement by the Federal government. SPECTROSCOPY AND THE STARS CONTENTS 2 Electromagnetic Ruler: The ER Ruler 3 The Rydberg Equation 4 Absorption Spectrum 5 Fraunhofer Lines In The Solar Spectrum 6 Dwarf Star Spectra 7 Stellar Spectra 8 Wien’s Displacement Law 8 Cosmic Background Radiation 9 Doppler Effect 10 Spectral Line profi les 11 Red Shifts 12 Red Shift 13 Hertzsprung-Russell Diagram 14 Parallax 15 Ladder of Distances 1 SPECTROSCOPY AND THE STARS ELECTROMAGNETIC RADIATION RULER: THE ER RULER Energy Level Transition Energy Wavelength RF = Radio frequency radiation µW = Microwave radiation nm Joules IR = Infrared radiation 10-27 VIS = Visible light radiation 2 8 UV = Ultraviolet radiation 4 6 6 RF 4 X = X-ray radiation Nuclear and electron spin 26 10- 2 γ = gamma ray radiation 1010 25 10- 109 10-24 108 µW 10-23 Molecular rotations 107 10-22 106 10-21 105 Molecular vibrations IR 10-20 104 SPACE INFRARED TELESCOPE FACILITY 10-19 103 VIS HUBBLE SPACE Valence electrons 10-18 TELESCOPE 102 Middle-shell electrons 10-17 UV 10 10-16 CHANDRA X-RAY 1 OBSERVATORY Inner-shell electrons 10-15 X 10-1 10-14 10-2 10-13 10-3 Nuclear 10-12 γ 10-4 COMPTON GAMMA RAY OBSERVATORY 10-11 10-5 6 4 10-10 2 2 -6 4 10 6 8 2 SPECTROSCOPY AND THE STARS THE RYDBERG EQUATION The wavelengths of one electron atomic emission spectra can be calculated from the Use the Rydberg equation to fi nd the wavelength ot Rydberg equation: the transition from n = 4 to n = 3 for singly ionized helium. -
The Formation and Early Evolution of Very Low-Mass Stars and Brown Dwarfs Held at ESO Headquarters, Garching, Germany, 11–14 October 2011
Astronomical News and spectroscopic surveys identifying the at the ELTs, together with encouraging emphasised the power of emerging coun- first galaxies, rare quasars, supernovae some explicitly high-risk projects. It was tries and public outreach for investments and gamma-ray bursts. noted that is very important to retain a in astronomical research and that diver- broad range of facilities, including sity in facilities and astronomical capabili- A lively discussion arose on data policy 4-metre- and 8-metre-class telescopes, ties should be retained together with and data mining for surveys and ELTs. to be used as survey facilities, to pro- large-scale projects. Ellis reminded us Most participants agreed that proprietary mote small projects, and to train young that we cannot plan the future in detail time should be at the minimum level but astronomers. All the long-term flagship and so optimism, versatility and creativity sufficient to guarantee intellectual owner- projects should try to involve more stu- remain the key attributes for success. ship and a satisfactory progress of the dents and young researchers, allowing surveys and the ELTs. Others proposed them to attend science working com- All the presentations and the conference to have the data public from the begin- mittees, and communicating the outcome picture are available at the conference ning. In order to facilitate data mining, it of the major high-level decisional meet- website: http://www.eso.org/sci/meetings/ was proposed that all data provided by ings to them. Furthermore, it was pro- 2011/feedgiant. the surveys and the ELTs should be Vir- posed that at least one young astrono- tual Observatory compliant from the out- mer should be included in each of the set. -
AST301 the Lives of the Stars
AST301 The Lives of the Stars A Tale of Two Forces: Pressure vs Gravity I. The Sun as a Star What we know about the Sun •Angular Diameter: q = 32 arcmin (from observations) •Solar Constant: f = 1.4 x 106 erg/sec/cm2 (from observations) •Distance: d = 1.5 x 108 km (1 AU). (from Kepler's Third Law and the trigonometric parallax of Venus) •Luminosity: L = 4 x 1033 erg/s. (from the inverse-square law: L = 4p d2 f) •Radius: R = 7 x 105 km. (from geometry: R = p d) •Mass: M = 2 x 1033 gm. (from Newton's version of Kepler's Third Law, M = (4p2/G) d3/P2) •Temperature: T = 5800 K. (from the black body law: L = 4pR2 σ T4) •Composition: about 74% Hydrogen, 24% Helium, and 2% everything else (by mass). (from spectroscopy) What Makes the Sun Shine? Inside the Sun Far Side Gary Larson Possible Sources of Sunlight • Chemical combustion – A Sun made of C+O: 4000 years • Gravitational Contraction – Convert gravitational potential energy – T = U/L = GM82R8/L8 ~ 107 years • Accretion – Limitless, but M8 increases 3% / 106 years • Nuclear Fusion – Good for ~1010 years How Fusion Works E=mc2 • 4 H ⇒ He4 + energy • The mass of 4 H atoms exceeds the mass of a He atom by 0.7%. • Every second, the Sun converts 6x108 tons of H into 5.96x108 tons of He. • The Sun loses 4x106 tons of mass every second. • At this rate, the Sun can maintain its present luminosity for about 1011 years. • 1010 or 1011 years ??? Nuclear Fusion Proton-Proton (PP I) reaction Releases 26.7 MeV 10 < Tcore < 14 MK How Fusion Works Source: Wikipedia Beyond PP I PP II: dominates for 14 < Tcore < 23 MK • 3He + 4He ⇒ 7Be + g 7 - 7 • Be + e ⇒ Li + ne + g • 7Li +p+ ⇒ 24He + g • 16% of L8 PP III: dominates for Tcore > 23 MK • 3He + 4He ⇒ 7Be + g • 7Be + p+ ⇒ 8B + g 8 8 + • B ⇒ Be + e + ne • 8Be ⇒ 24He • 0.02% of L8 Nuclear Timescale • 1010 years • Sun has brightened by 30% in 4.5 Gyr • Photons take 105 – 106 yrs to diffuse out – Gamma-rays thermalize to optical photons How do we know? • The p-p reaction also produces neutrinos. -
Calibration Against Spectral Types and VK Color Subm
Draft version July 19, 2021 Typeset using LATEX default style in AASTeX63 Direct Measurements of Giant Star Effective Temperatures and Linear Radii: Calibration Against Spectral Types and V-K Color Gerard T. van Belle,1 Kaspar von Braun,1 David R. Ciardi,2 Genady Pilyavsky,3 Ryan S. Buckingham,1 Andrew F. Boden,4 Catherine A. Clark,1, 5 Zachary Hartman,1, 6 Gerald van Belle,7 William Bucknew,1 and Gary Cole8, ∗ 1Lowell Observatory 1400 West Mars Hill Road Flagstaff, AZ 86001, USA 2California Institute of Technology, NASA Exoplanet Science Institute Mail Code 100-22 1200 East California Blvd. Pasadena, CA 91125, USA 3Systems & Technology Research 600 West Cummings Park Woburn, MA 01801, USA 4California Institute of Technology Mail Code 11-17 1200 East California Blvd. Pasadena, CA 91125, USA 5Northern Arizona University Department of Astronomy and Planetary Science NAU Box 6010 Flagstaff, Arizona 86011, USA 6Georgia State University Department of Physics and Astronomy P.O. Box 5060 Atlanta, GA 30302, USA 7University of Washington Department of Biostatistics Box 357232 Seattle, WA 98195-7232, USA 8Starphysics Observatory 14280 W. Windriver Lane Reno, NV 89511, USA (Received April 18, 2021; Revised June 23, 2021; Accepted July 15, 2021) Submitted to ApJ ABSTRACT We calculate directly determined values for effective temperature (TEFF) and radius (R) for 191 giant stars based upon high resolution angular size measurements from optical interferometry at the Palomar Testbed Interferometer. Narrow- to wide-band photometry data for the giants are used to establish bolometric fluxes and luminosities through spectral energy distribution fitting, which allow for homogeneously establishing an assessment of spectral type and dereddened V0 − K0 color; these two parameters are used as calibration indices for establishing trends in TEFF and R. -
Stellar Evolution
Stellar Astrophysics: Stellar Evolution 1 Stellar Evolution Update date: December 14, 2010 With the understanding of the basic physical processes in stars, we now proceed to study their evolution. In particular, we will focus on discussing how such processes are related to key characteristics seen in the HRD. 1 Star Formation From the virial theorem, 2E = −Ω, we have Z M 3kT M GMr = dMr (1) µmA 0 r for the hydrostatic equilibrium of a gas sphere with a total mass M. Assuming that the density is constant, the right side of the equation is 3=5(GM 2=R). If the left side is smaller than the right side, the cloud would collapse. For the given chemical composition, ρ and T , this criterion gives the minimum mass (called Jeans mass) of the cloud to undergo a gravitational collapse: 3 1=2 5kT 3=2 M > MJ ≡ : (2) 4πρ GµmA 5 For typical temperatures and densities of large molecular clouds, MJ ∼ 10 M with −1=2 a collapse time scale of tff ≈ (Gρ) . Such mass clouds may be formed in spiral density waves and other density perturbations (e.g., caused by the expansion of a supernova remnant or superbubble). What exactly happens during the collapse depends very much on the temperature evolution of the cloud. Initially, the cooling processes (due to molecular and dust radiation) are very efficient. If the cooling time scale tcool is much shorter than tff , −1=2 the collapse is approximately isothermal. As MJ / ρ decreases, inhomogeneities with mass larger than the actual MJ will collapse by themselves with their local tff , different from the initial tff of the whole cloud. -
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. -
Atoms and Astronomy
Atoms and Astronomy n If O o p W H- I on-* C3 W KJ CD NASA National Aeronautics and Space Administration ATOMS IN ASTRONOMY A curriculum project of the American Astronomical Society, prepared with the cooperation of the National Aeronautics and Space Administration and the National Science Foundation : by Paul A. Blanchard f Theoretical Studies Group *" NASA Goddard Space Flight Center Greenbelt, Maryland National Aeronautics and Space Administration Washington, DC 20546 September 1976 For sale by the Superintendent of Documents, U.S. Government Printing Office Washington, D.C. 20402 - Price $1.20 Stock No. 033-000-00656-0/Catalog No. NAS 1.19:128 intenti PREFACE In the past half century astronomers have provided mankind with a new view of the universe, with glimpses of the nature of infinity and eternity that beggar the imagination. Particularly, in the past decade, NASA's orbiting spacecraft as well as ground-based astronomy have brought to man's attention heavenly bodies, sources of energy, stellar and galactic phenomena, about the nature of which the world's scientists can only surmise. Esoteric as these new discoveries may be, astronomers look to the anticipated Space Telescope to provide improved understanding of these phenomena as well as of the new secrets of the cosmos which they expect it to unveil. This instrument, which can observe objects up to 30 to 100 times fainter than those accessible to the most powerful Earth-based telescopes using similar techniques, will extend the use of various astronomical methods to much greater distances. It is not impossible that observations with this telescope will provide glimpses of some of the earliest galaxies which were formed, and there is a remoter possibility that it will tell us something about the edge of the universe.