Astronomy 2017 Princeton University Invitational
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Cygnus OB2 – a Young Globular Cluster in the Milky Way Jürgen Knödlseder
Cygnus OB2 – a young globular cluster in the Milky Way Jürgen Knödlseder To cite this version: Jürgen Knödlseder. Cygnus OB2 – a young globular cluster in the Milky Way. Astronomy and Astrophysics - A&A, EDP Sciences, 2000, 360, pp.539 - 548. hal-01381935 HAL Id: hal-01381935 https://hal.archives-ouvertes.fr/hal-01381935 Submitted on 14 Oct 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Astron. Astrophys. 360, 539–548 (2000) ASTRONOMY AND ASTROPHYSICS Cygnus OB2–ayoung globular cluster in the Milky Way J. Knodlseder¨ INTEGRAL Science Data Centre, Chemin d’Ecogia 16, 1290 Versoix, Switzerland Centre d’Etude Spatiale des Rayonnements, CNRS/UPS, B.P. 4346, 31028 Toulouse Cedex 4, France ([email protected]) Received 31 May 2000 / Accepted 23 June 2000 Abstract. The morphology and stellar content of the Cygnus particularly good region to address such questions, since it is OB2 association has been determined using 2MASS infrared extremely rich (e.g. Reddish et al. 1966, hereafter RLP), and observations in the J, H, and K bands. The analysis reveals contains some of the most luminous stars known in our Galaxy a spherically symmetric association of ∼ 2◦ in diameter with (e.g. -
POSTERS SESSION I: Atmospheres of Massive Stars
Abstracts of Posters 25 POSTERS (Grouped by sessions in alphabetical order by first author) SESSION I: Atmospheres of Massive Stars I-1. Pulsational Seeding of Structure in a Line-Driven Stellar Wind Nurdan Anilmis & Stan Owocki, University of Delaware Massive stars often exhibit signatures of radial or non-radial pulsation, and in principal these can play a key role in seeding structure in their radiatively driven stellar wind. We have been carrying out time-dependent hydrodynamical simulations of such winds with time-variable surface brightness and lower boundary condi- tions that are intended to mimic the forms expected from stellar pulsation. We present sample results for a strong radial pulsation, using also an SEI (Sobolev with Exact Integration) line-transfer code to derive characteristic line-profile signatures of the resulting wind structure. Future work will compare these with observed signatures in a variety of specific stars known to be radial and non-radial pulsators. I-2. Wind and Photospheric Variability in Late-B Supergiants Matt Austin, University College London (UCL); Nevyana Markova, National Astronomical Observatory, Bulgaria; Raman Prinja, UCL There is currently a growing realisation that the time-variable properties of massive stars can have a funda- mental influence in the determination of key parameters. Specifically, the fact that the winds may be highly clumped and structured can lead to significant downward revision in the mass-loss rates of OB stars. While wind clumping is generally well studied in O-type stars, it is by contrast poorly understood in B stars. In this study we present the analysis of optical data of the B8 Iae star HD 199478. -
Sky Notes by Neil Bone 2005 August & September
Sky notes by Neil Bone 2005 August & September below Castor and Pollux. Mercury is soon ing June and July, it is still quite possible that Sun and Moon lost from view again, arriving at superior con- noctilucent clouds (NLC) could be seen into junction beyond the Sun on September 18. early August, particularly by observers at The Sun continues its southerly progress along Venus continues its rather unfavourable more northerly locations. Quite how late into the ecliptic, reaching the autumnal equinox showing as an ‘Evening Star’. Although it August NLC can be seen remains to be deter- position at 22h 23m Universal Time (UT = pulls out to over 40° elongation east of the mined: there have been suggestions that the GMT; BST minus 1 hour) on September 22. Sun during September, Venus is also heading visibility period has become longer in recent At that precise time, the centre of the solar southwards, and as a result its setting-time years. Observational reports will be welcomed disk is positioned at the intersection between after the Sun remains much the same − barely by the Aurora Section. the celestial equator and the ecliptic, the latter an hour − during this interval. Although bright While declining sunspot activity makes great circle on the sky being inclined by 23.5° at magnitude −4, Venus will be quite tricky major aurorae extending to lower latitudes to the former. Calendrical autumn begins at the to catch in the early twilight: viewing cir- less likely, the appearance of coronal holes equinox, but amateur astronomers might more cumstances don’t really improve until the in the latter parts of the cycle does bring the readily follow meteorological timing, wherein closing weeks of 2005. -
The E-MERLIN 21 Cm Legacy Survey of Cygnus OB2
This is a repository copy of COBRaS: The e-MERLIN 21 cm Legacy survey of Cygnus OB2. White Rose Research Online URL for this paper: http://eprints.whiterose.ac.uk/162252/ Version: Published Version Article: Morford, JC, Fenech, DM, Prinja, RK et al. (12 more authors) (2020) COBRaS: The e-MERLIN 21 cm Legacy survey of Cygnus OB2. Astronomy & Astrophysics, 637. A64. ISSN 0004-6361 https://doi.org/10.1051/0004-6361/201731379 Reuse Items deposited in White Rose Research Online are protected by copyright, with all rights reserved unless indicated otherwise. They may be downloaded and/or printed for private study, or other acts as permitted by national copyright laws. The publisher or other rights holders may allow further reproduction and re-use of the full text version. This is indicated by the licence information on the White Rose Research Online record for the item. Takedown If you consider content in White Rose Research Online to be in breach of UK law, please notify us by emailing [email protected] including the URL of the record and the reason for the withdrawal request. [email protected] https://eprints.whiterose.ac.uk/ A&A 637, A64 (2020) https://doi.org/10.1051/0004-6361/201731379 Astronomy c ESO 2020 & Astrophysics COBRaS: The e-MERLIN 21 cm Legacy survey of Cygnus OB2 J. C. Morford1, D. M. Fenech1,2, R. K. Prinja1, R. Blomme3, J. A. Yates1, J. J. Drake4, S. P. S. Eyres5,6, A. M. S. Richards7, I. R. Stevens8, N. J. Wright9, J. S. Clark10, S. -
Useful Constants
Appendix A Useful Constants A.1 Physical Constants Table A.1 Physical constants in SI units Symbol Constant Value c Speed of light 2.997925 × 108 m/s −19 e Elementary charge 1.602191 × 10 C −12 2 2 3 ε0 Permittivity 8.854 × 10 C s / kgm −7 2 μ0 Permeability 4π × 10 kgm/C −27 mH Atomic mass unit 1.660531 × 10 kg −31 me Electron mass 9.109558 × 10 kg −27 mp Proton mass 1.672614 × 10 kg −27 mn Neutron mass 1.674920 × 10 kg h Planck constant 6.626196 × 10−34 Js h¯ Planck constant 1.054591 × 10−34 Js R Gas constant 8.314510 × 103 J/(kgK) −23 k Boltzmann constant 1.380622 × 10 J/K −8 2 4 σ Stefan–Boltzmann constant 5.66961 × 10 W/ m K G Gravitational constant 6.6732 × 10−11 m3/ kgs2 M. Benacquista, An Introduction to the Evolution of Single and Binary Stars, 223 Undergraduate Lecture Notes in Physics, DOI 10.1007/978-1-4419-9991-7, © Springer Science+Business Media New York 2013 224 A Useful Constants Table A.2 Useful combinations and alternate units Symbol Constant Value 2 mHc Atomic mass unit 931.50MeV 2 mec Electron rest mass energy 511.00keV 2 mpc Proton rest mass energy 938.28MeV 2 mnc Neutron rest mass energy 939.57MeV h Planck constant 4.136 × 10−15 eVs h¯ Planck constant 6.582 × 10−16 eVs k Boltzmann constant 8.617 × 10−5 eV/K hc 1,240eVnm hc¯ 197.3eVnm 2 e /(4πε0) 1.440eVnm A.2 Astronomical Constants Table A.3 Astronomical units Symbol Constant Value AU Astronomical unit 1.4959787066 × 1011 m ly Light year 9.460730472 × 1015 m pc Parsec 2.0624806 × 105 AU 3.2615638ly 3.0856776 × 1016 m d Sidereal day 23h 56m 04.0905309s 8.61640905309 -
Metadata of the Chapter That Will Be Visualized Online
Metadata of the chapter that will be visualized online Chapter Title Binary Systems and Their Nuclear Explosions Copyright Year 2018 Copyright Holder The Author(s) Author Family Name Isern Particle Given Name Jordi Suffix Organization Institute of Space Sciences (ICE, CSIC) Address Barcelona, Spain Organization Institut d’Estudis Espacials de Catalunya (IEEC) Address Barcelona, Spain Email [email protected] Corresponding Author Family Name Hernanz Particle Given Name Margarita Suffix Organization Institute of Space Sciences (ICE, CSIC) Address Barcelona, Spain Organization Institut d’Estudis Espacials de Catalunya (IEEC) Address Barcelona, Spain Email [email protected] Author Family Name José Particle Given Name Jordi Suffix Organization Universitat Politècnica de Catalunya (UPC) Address Barcelona, Spain Organization Institut d’Estudis Espacials de Catalunya (IEEC) Address Barcelona, Spain Email [email protected] Abstract The nuclear energy supply of a typical star like the Sun would be ∼ 1052 erg if all the hydrogen could be incinerated into iron peak elements. Chapter 5 1 Binary Systems and Their Nuclear 2 Explosions 3 Jordi Isern, Margarita Hernanz, and Jordi José 4 5.1 Accretion onto Compact Objects and Thermonuclear 5 Runaways 6 The nuclear energy supply of a typical star like the Sun would be ∼1052 erg if all 7 the hydrogen could be incinerated into iron peak elements. Since the gravitational 8 binding energy is ∼1049 erg, it is evident that the nuclear energy content is more 9 than enough to blow up the Sun. However, stars are stable thanks to the fact that their 10 matter obeys the equation of state of a classical ideal gas that acts as a thermostat: if 11 some energy is released as a consequence of a thermal fluctuation, the gas expands, 12 the temperature drops and the instability is quenched. -
Diffuse X-Ray Emission in the Cygnus OB2 Association
to appear in special issue ApJSS., 2018 Preprint typeset using LATEX style AASTeX6 v. 1.0 DIFFUSE X-RAY EMISSION IN THE CYGNUS OB2 ASSOCIATION. J. F. Albacete Colombo1, J. J. Drake2,E.Flaccomio3,N.J.Wright4, V. Kashyap2,M.G.Guarcello3,K.Briggs5,J.E.Drew6, D. M. Fenech7,G.Micela3, M. McCollough2,R.K.Prinja7,N.Schneider8,S.Sciortino3,J.S.Vink9 1Universidad de R´ıo Negro, Sede Atl´antica, Viedma CP8500, Argentina. 2Smithsonian Astrophysical Observatory, 60 Garden St., Cambridge, MA 02138, U.S.A 3INAF-Osservatorio Astronomico di Palermo, Piazza del Parlamento 1, 90134 Palermo, Italy. 4Astrophysics Group, Keele University, Keele, Staffordshire ST5 5BG, UK. 5Hamburger Sternwarte, University of Hamburg, Gojenbergsweg 112, 21029, Hamburg, Germany. 6School of Physics, Astronomy & Mathematics, University of Hertfordshire, College Lane, Hatfield, Hertfordshire, AL10 9AB, UK. 7Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK. 8I. Physik. Institut, University of Cologne, D-50937 Cologne, Germany. 9Armagh Observatory and Planetarium, College Hill, Armagh BT61 9DG, Northern Ireland, UK. ABSTRACT We present a large-scale study of diffuse X-ray emission in the nearby massive stellar association Cygnus OB2 as part of the Chandra Cygnus OB2 Legacy Program. We used 40 Chandra X-ray ACIS-I observations covering ∼1.0 deg2. After removing 7924 point-like sources detected in our survey, background-corrected X-ray emission, the adaptive smoothing reveals large-scale diffuse X-ray emission. Diffuse emission was de- tected in the sub-bands Soft [0.5:1.2] and Medium [1.2:2.5], and marginally in the Hard [2.5:7.0] keV band. -
Nobel Lecture: Accelerating Expansion of the Universe Through Observations of Distant Supernovae*
REVIEWS OF MODERN PHYSICS, VOLUME 84, JULY–SEPTEMBER 2012 Nobel Lecture: Accelerating expansion of the Universe through observations of distant supernovae* Brian P. Schmidt (published 13 August 2012) DOI: 10.1103/RevModPhys.84.1151 This is not just a narrative of my own scientific journey, but constant, and suggested that Hubble’s data and Slipher’s also my view of the journey made by cosmology over the data supported this conclusion (Lemaˆitre, 1927). His work, course of the 20th century that has lead to the discovery of the published in a Belgium journal, was not initially widely read, accelerating Universe. It is complete from the perspective of but it did not escape the attention of Einstein who saw the the activities and history that affected me, but I have not tried work at a conference in 1927, and commented to Lemaˆitre, to make it an unbiased account of activities that occurred ‘‘Your calculations are correct, but your grasp of physics is around the world. abominable.’’ (Gaither and Cavazos-Gaither, 2008). 20th Century Cosmological Models: In 1907 Einstein had In 1928, Robertson, at Caltech (just down the road from what he called the ‘‘wonderful thought’’ that inertial accel- Edwin Hubble’s office at the Carnegie Observatories), pre- eration and gravitational acceleration were equivalent. It took dicted the Hubble law, and claimed to see it when he com- Einstein more than 8 years to bring this thought to its fruition, pared Slipher’s redshift versus Hubble’s galaxy brightness his theory of general Relativity (Norton and Norton, 1984)in measurements, but this observation was not substantiated November, 1915. -
Spectroscopy of 13 High Mass Stars in the Cyg OB2 Association
will be published in Astronomy Reports, 2013, vol. 67, No. 7 Spectroscopy of 13 high mass stars in the Cyg OB2 association E.L. Chentsov, V.G. Klochkova, V.E. Panchuk, M.V. Yushkin Special Astrophysical Observatory RAS, Nizhnij Arkhyz, Russia March 15, 2018 Abstract Aiming to explore weak spectral features of stellar and interstellar origin we used the NES echelle spectrograph of the 6–m telescope to obtain high–resolution spectra for 13 hot O3–B4 stars in the Cyg OB2 association, including a high luminous star No. 12. Velocity fields in the atmospheres and interstellar medium, characteristics of optical spectra and line profiles are investigated. The cascade star formation scheme for the association is confirmed. Evidence is presented suggesting that the hypergiant Cyg OB2 No. 12 is an LBV object and that its anomalous reddening has a circumstellar nature. 1. Introduction Among hypergiants of the Galaxy, those belonging to stellar associations are most attractive for study. Membership in a stellar group makes it easier to estimate a stars age, luminosity, and center of mass radial velocity, which is needed to introduce a zero point for the system of velocities observed in the stellar atmosphere and wind. In addition, studies of stars with extreme luminosities and mass loss rates can naturally be expanded to their influence on the associations gas and dust component and the star formation process. In the present paper, we address this two-sided problem for the enigmatic star No. 12 and other members h m of the Cyg OB2 association. This association (initially named VI Cyg; α2000 = 20 33.2 , o o o δ2000 = +41.32 , l = 80.2 , b = +0.8 ) was discovered in the middle of the 20-th century and still remains one of the most actively studied objects in our Galaxy. -
Stars and Their Spectra: an Introduction to the Spectral Sequence Second Edition James B
Cambridge University Press 978-0-521-89954-3 - Stars and Their Spectra: An Introduction to the Spectral Sequence Second Edition James B. Kaler Index More information Star index Stars are arranged by the Latin genitive of their constellation of residence, with other star names interspersed alphabetically. Within a constellation, Bayer Greek letters are given first, followed by Roman letters, Flamsteed numbers, variable stars arranged in traditional order (see Section 1.11), and then other names that take on genitive form. Stellar spectra are indicated by an asterisk. The best-known proper names have priority over their Greek-letter names. Spectra of the Sun and of nebulae are included as well. Abell 21 nucleus, see a Aurigae, see Capella Abell 78 nucleus, 327* ε Aurigae, 178, 186 Achernar, 9, 243, 264, 274 z Aurigae, 177, 186 Acrux, see Alpha Crucis Z Aurigae, 186, 269* Adhara, see Epsilon Canis Majoris AB Aurigae, 255 Albireo, 26 Alcor, 26, 177, 241, 243, 272* Barnard’s Star, 129–130, 131 Aldebaran, 9, 27, 80*, 163, 165 Betelgeuse, 2, 9, 16, 18, 20, 73, 74*, 79, Algol, 20, 26, 176–177, 271*, 333, 366 80*, 88, 104–105, 106*, 110*, 113, Altair, 9, 236, 241, 250 115, 118, 122, 187, 216, 264 a Andromedae, 273, 273* image of, 114 b Andromedae, 164 BDþ284211, 285* g Andromedae, 26 Bl 253* u Andromedae A, 218* a Boo¨tis, see Arcturus u Andromedae B, 109* g Boo¨tis, 243 Z Andromedae, 337 Z Boo¨tis, 185 Antares, 10, 73, 104–105, 113, 115, 118, l Boo¨tis, 254, 280, 314 122, 174* s Boo¨tis, 218* 53 Aquarii A, 195 53 Aquarii B, 195 T Camelopardalis, -
Type Ia Supernovaeof Are a the Outc Carbon–Oxygen White Dwarf in a Binary System
Type Ia Supernova: Observations and Theory PoS(NIC XI)066 Jordi Isern∗ Institute for Space Sciences (CSIC-IEEC) E-mail: [email protected] Eduardo Bravo Department of Nuclear Physics (UPC)/IEEC E-mail: [email protected] Alina Hirschmann Institute for Space Sciences (CSIC-IEEC) E-mail: [email protected] There is a wide consensus that Type Ia supernovae are the outcome of the thermonuclear explosion of a carbon–oxygen white dwarf in a binary system. Nevertheless, the nature of this system, the process of ignition itself and the development of the explosion continue to be a mystery despite the important improvements that both, theory and observations, have experienced during the last years. Furthermore, the discovery of new events that are challenging the classical scenario forces the exploration of new issues or, at least, to reconsider scenarios that were rejected at a given moment. 11th Symposium on Nuclei in the Cosmos 19-23 July 2010 Heidelberg, Germany. ∗Speaker. c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence. http://pos.sissa.it/ Type Ia Supernova: Observations and Theory Jordi Isern 1. Introduction Supernovae are characterized by a sudden rise of their luminosity, by a steep decline after maximum light that lasts several weeks, followed by an exponential decline that can last several years. The total electromagnetic output, obtained from the light curve, is ∼ 1049 erg, while the 10 luminosity at maximum can be as high as ∼ 10 L⊙. The kinetic energy of supernovae can be estimated from the expansion velocity of the ejecta, vexp ∼ 5,000 − 10,000 km/s, and turns out to be ∼ 1051 erg. -
Homework 6 – Stellar Physics 1. Cygnus X-1 Is an X-Ray Source In
Homework 6 – Stellar Physics 1. Cygnus X-1 is an x-ray source in the constellation Cygnus that astrophysicists believe is a black hole. An artist’s impression is shown in Figure 1A. Figure 1A The mass of the black hole has been determined to be 14∙8 solar masses. (a) (i) State what is meant by the Schwarzschild radius of a black hole. (ii) Calculate the Schwarzchild radius of the black hole in Cygnus X-1. (b) The Hertzsprung-Russell (H-R) diagram shown in Figure 1B shows the relationship between luminosity and surface temperature of stars. Figure 1B Zeta Cygni B and Chi Cygni are two stars in the constellation Cygnus. They are shown on the H-R diagram. Chi Cygni is more luminous than Zeta Cygni B. Describe two other differences between these stars. (c) Another star, Aldebaran B, is a distance of 6∙16 x 1017 m from the Earth. The luminosity of Aldebaran B is 2∙32 x 1025 W and its temperature is determined to be 3∙4 x 103 K. (i) Calculate the radius of Aldebaran B. (ii) Calculate the apparent brightness of Aldebaran B as observed from Earth. 1 2. Hertzsprung-Russell (H-R) diagrams are widely used by physicists and astronomers to categorise stars. Figure 2A shows a simplified H-R diagram. Figure 2A (a) State what class of star Sirius B is. (b) Estimate the radius of Betelgeuse. (c) Ross 128 and Barnard’s Star have a similar temperature but Barnard’s Star has a slightly greater luminosity. Determine what other information this tells you about the two stars.