Mass Loss from Hot Massive Stars
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Type Ia Supernovae, Massive White Dwarfs, and Ap Stars
Merging of Components in Close Binaries: Type Ia Supernovae, Massive White Dwarfs, and Ap stars A. I. Bogomazov1, A. V. Tutukov2 1 Sternberg Astronomical Institute, Moscow State University, Universitetski pr. 13, Moscow, 119992, Russia, 2 Institute of Astronomy, Russian Academy of Sciences, ul. Pyatnitskaya 48, Moscow, 109017, Russia Astronomy Reports, volume 53, no. 3, pp. 214-222 (2009) The “Scenario Machine” (a computer code designed for studies of the evolution of close bina- ries) was used to carry out a population synthesis for a wide range of merging astrophysical objects: main-sequence stars with main-sequence stars; white dwarfs with white dwarfs, neu- tron stars, and black holes; neutron stars with neutron stars and black holes; and black holes with black holes.We calculate the rates of such events, and plot the mass distributions for merging white dwarfs and main-sequence stars. It is shown that Type Ia supernovae can be used as standard candles only after approximately one billion years of evolution of galaxies. In the course of this evolution, the average energy of Type Ia supernovae should decrease by roughly 10%; the maximum and minimum energies of Type Ia supernovae may differ by no less than by a factor of 1.5. This circumstance should be taken into account in estimations of parameters of acceleration of the Universe. According to theoretical estimates, the most massive – as a rule, magnetic – white dwarfs probably originate from mergers of white dwarfs of lower mass. At least some magnetic Ap and Bp stars may form in mergers of low-mass main-sequence stars (M . -
A Synchrotron Superbubble in the IC 10 Galaxy: a Hypernova Remnant?
Mon. Not. R. Astron. Soc. 000, 1–?? (2007) Printed 28 October 2018 (MN LATEX style file v2.2) A synchrotron superbubble in the IC 10 Galaxy: a hypernova remnant? T. A. Lozinskaya1⋆ and A. V. Moiseev2 1Sternberg Astronomical Institute, Universitetskii pr. 13, Moscow, 119991 Russia 2Special Astrophysical Observatory, Nizhnii Arkhyz, Karachaevo-Cherkesia, 369167 Russia Accepted 2007 June 29. Received 2007 June; in original form 2007 June 4 ABSTRACT The nature of the synchrotron superbubble in the IC 10 galaxy is discussed using the results of our investigation of its ionized gas structure, kinematics, and emission spectrum from observations made with the 6-m telescope of the Special Astrophysical Observatory of the Russian Academy of Sciences, and based on our analysis of the radio emission of the region. The hypernova explosion is shown to be a more plausi- ble mechanism of the formation of the synchrotron superbubble compared with the earlier proposed model of multiple supernova explosions. A compact remnant of this hypernova may be identified with the well known X-ray binary X-1 – an accreting black hole. Key words: ISM: bubbles – ISM: kinematics and dynamics – supernova remnants galaxies: individual: IC 10. 1 INTRODUCTION. and observations with a scanning Fabry–Perot interferom- eter (FPI) in the Hα line. We report the detailed results The synchrotron superbubble in the IC 10 galaxy was discov- of our observations in a separate paper (Lozinskaya et al. ered by Yang & Skillman (1993). They associated it with the 2007). In this Letter we summarize the main results of these explosion of about ten supernovae. The synchrotron nature observations and the ensuing conclusions. -
Multi-Periodic Photospheric Pulsations and Connected Wind Structures in HD 64760
A&A 447, 325–341 (2006) Astronomy DOI: 10.1051/0004-6361:20053847 & c ESO 2006 Astrophysics Multi-periodic photospheric pulsations and connected wind structures in HD 64760 A. Kaufer1,O.Stahl2,R.K.Prinja3, and D. Witherick3, 1 European Southern Observatory, Alonso de Cordova 3107, Casilla 19001, Santiago 19, Chile e-mail: [email protected] 2 Landessternwarte Heidelberg, Königstuhl 12, 69117 Heidelberg, Germany 3 Department of Physics & Astronomy, University College London, Gower Street, London, WC1E 6BT, UK Received 18 July 2005 / Accepted 17 October 2005 ABSTRACT We report on the results of an extended optical spectroscopic monitoring campaign on the early-type B supergiant HD 64760 (B0.5 Ib) designed to probe the deep-seated origin of spatial wind structure in massive stars. This new study is based on high-resolution echelle spectra obtained with the Feros instrument at ESO La Silla. 279 spectra were collected over 10 nights between February 14 and 24, 2003. From the period analysis of the line-profile variability of the photospheric lines we identify three closely spaced periods around 4.810 h and a splitting of ±3%. The velocity – phase diagrams of the line-profile variations for the distinct periods reveal characteristic prograde non-radial pulsation patterns of high order corresponding to pulsation modes with l and m in the range 6−10. A detailed modeling of the multi-periodic non-radial pulsations with the Bruce and Kylie pulsation-model codes (Townsend 1997b, MNRAS, 284, 839) favors either three modes with l = −m and l = 8, 6, 8 or m = −6andl = 8, 6, 10 with the second case maintaining the closely spaced periods in the co-rotating frame. -
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. -
Annual Report 2008
Koninklijke Sterrenwacht van België Observatoire royal de Belgique Royal Observatory of Belgium Mensen voor Aarde en Ruimte , Aarde en Ruimte voor Mensen Des hommes et des femmes pour la Terre et l'Espace, La Terre et l'Espace pour l'Homme Jaarverslag 2008 Rapport Annuel 2008 Annual Report 2008 De activiteiten beschreven in dit verslag werden ondersteund door Les activités décrites dans ce rapport ont été soutenues par The activities described in this report were supported by De POD Wetenschapsbeleid / Le SPP Politique Scientifique De Nationale Loterij La Loterie Nationale De Europese Gemeenschap Het Europees Ruimtevaartagentschap La Communauté Européenne L’Agence Spatiale Européenne Het Fond voor Wetenschappelijk Onderzoek Le Fonds de la Recherche Scientifique – Vlaanderen Le Fonds pour la formation à la Recherche dans l’Industrie et dans l’Agriculture (FRIA) Instituut voor de aanmoediging van innovatie door Wetenschap & Technologie in Vlaanderen Privé-sponsoring door Mr. G. Berthault / Sponsoring privé par M. G. Berthault 2 Deel 1: Wetenschappelijke activiteiten Partie 1: Activités Scientifiques Part 1: Scientific Activities 3 4 Summary Abbreviations.................................................................................................................................. 7 A. GNSS Positioning and Time............................................................................................. 14 A.1. Time and Time transfer .............................................................................................................15 -
La Photosynthèse Serait Apparue Chez Certains Organismes Primitifs Entre 2.800 Et -2.400 Millions D’Années Si L’On En Croit Certaines Archives Géologiques Terrestres
La photosynthèse serait apparue chez certains organismes primitifs entre 2.800 et -2.400 millions d’années si l’on en croit certaines archives géologiques terrestres. Mais certains la font remonter bien plus tôt en faisant l’hypothèse que les stromatolites que l’on retrouve dans des couches plus anciennes encore sont bien le produit d’une activité biologique. Actuellement, nous n’en sommes sûrs que pour ceux datant de -2.724 millions d’années mais des stromatolites existaient déjà sur Terre il y a 3,5 milliards d’années environ. Quoiqu'il en soit, une certitude demeure, concernant les immenses dépôts de fer du bassin de Hamersley en Australie. Ils datent de l’époque du Sidérien alors que la surface des continents était devenue suffisamment importante pour que se forment des mers peu profondes entourées de grande plates-formes continentales. Les conditions étaient remplies pour que de grands tapis de bactéries construisent des stromatolites en quantités importantes et dégagent massivement de l’oxygène par photosynthèse. Ce gaz corrosif a alors pu oxyder le fer en solution dans les océans et entraîner sa précipitation sous forme d’hydroxyde de fer, de carbonate de fer, de silicate ou de sulfures, selon des variations de l’acidité et du degré d’oxydoréduction de l’eau de mer. C’est ce qu’on appelle la Grande oxydation ou la Catastrophe de l’oxygène. Vers -1.900 millions d’années, la presque totalité du fer présent dans les océans avait précipité et il se retrouve aujourd’hui dans les grands gisements de minerai mondiaux tels que ceux de Hamersley. -
Breaching the Eddington Limit in the Most Massive, Most Luminous Stars
Mass Loss from (Hot) Massive Luminous Stars Stan Owocki Bartol Research Institute Department of Physics & Astronomy University of Delaware Wednesday, January 12, 2011 Massive Stars in the Whirlpool Galaxy Wednesday, January 12, 2011 Henize 70: LMC SuperBubble Wind-Blown Bubbles in ISM Some key scalings: Wednesday, January 12, 2011 Henize 70: LMC SuperBubble Wind-Blown Bubbles in ISM Some key scalings: WR wind bubble NGC 2359 Wednesday, January 12, 2011 Henize 70: LMC SuperBubble Wind-Blown Bubbles in ISM Some key scalings: WR wind bubble NGC 2359 Superbubble in the Large Magellanic Cloud Wednesday, January 12, 2011 Pistol Nebula Wednesday, January 12, 2011 Eta Carinae Wednesday, January 12, 2011 P-Cygni Line Profile Line-scattering in massive winds Wednesday, January 12, 2011 Observed wind line profiles Resonance line-scattering Recombination line O-star P-Cygni profile WR-star emission profile −v∞ +v −v∞ ∞ Wednesday, January 12, 2011 Basic Mass Loss Properties i 2 Mass Loss rate M = 4πρvr Terminal speed Velocity law v(r) v∞ 8 Wednesday, January 12, 2011 Massive-Star Mass Loss i M 1. OB Winds M ~ 10−9 − 10−6 yr v∞ 1000 − 3000 km / s – opt. thin τ c < 1 2. Wolf-Rayet Winds i M M ~ 10−6 − 10−5 yr – opt. thick τ c > 1 v∞ 1000 − 3000 km / s 3. Luminous Blue Variable (LBV) Eruptions i 1 −5 M -very opt. thick τ c M ~ 10 − 1 !! yr v∞ 50 − 1000 km / s Wednesday, January 12, 2011 Q: What can drive such extreme mass loss?? Wednesday, January 12, 2011 Q: What can drive such extreme mass loss?? A: The force of light! Wednesday, January 12, 2011 -
Chapter 3 – Astrospheres, Stellar Winds, and the Interstellar Medium
3 Astrospheres, stellar winds, and the interstellar medium BRIAN E. WOOD AND JEFFREY L. LINSKY 3.1 The spatial extent of the solar wind While orbiting the Sun, the Earth and the other planers in our solar system are ex posed to an outflow of plasma from the Sun. This is the solar wi nd, which largely determines the particle environment of the planets, as well as their magnetospheric properties. Long-tenn exposure Lo the solar wind may have had signjficant cffectc; on planetary atmospheres in some cases. Mars is a particularly interesting example, as the Martian atmosphere was once much thicker than it is today, and the erosive effects of solar wind exposure are commonly believed to be responsible for itc; depletion (see Ch. 8; also Jakosky et al.. 1994; Atreya et al., 2013). The solar wind does not expand indefinitely. Eventually it runs into the inter stellar medium (ISM), the ex tre mely low-particle-density e nvironment that exists in between the stars. Our Sun is moving relative to the ISM that surrounds the planetary system, so we see a fl ow of interstellar matter in the heliocentric rest frame, coming from the direction of the constellation Ophiuchus. The interaction between the solar wind and the ISM flow determines the large-scale structure of our he liosphere. which basically defines the extent of the solar wind's reach into our Galactic environment. Other stars are naturally surrounded by their own "astro spheres" (allernatively "asterospheres"') defined by the strength of their own stellar winds, the nature of the ISM in their Galactic neighborhoods, and their rnlative motion. -
Modelling Supernova Remnant Kinematics and X-Ray Emission: Some Examples
Modelling Supernova Remnant kinematics and X-ray emission: Some Examples. Margarita Rosado Instituto de Astronomía UNAM Collaborators: • Pablo Velázquez, Ary Rodríguez González (ICN-UNAM) • Jorge Reyes Iturbide (IT Santiago Tianguistengo) • Patricia Ambrocio-Cruz (UAEH) • Mónica Sánchez-Cruces (ESFM-IPN) I. The Kinematics: By means of a FP Interferometer (i.e. the PUMA) One gets millions of Halpha or [SII] profiles over the field. From Valdez- Gutiérrez et al. 2001 OAN: San Pedro Mártir, B.C. Mexico PUMA INTERFEROMETER PUMA parameters - Detector CCD 1024x1024 – FP scanning steps 48 – Finesse 24 – Spectral resolution 47.3 km s-1 – Plate scale 0.59 arcsec pix -1 – Filters Hα [SII] – Central lambda a 6570 6720 – Interference order 330 332 – Free spectral range b 847 931 – Sampling step c 17.6 19.4 – Calibration line a Hα (6562.7) Ne (6717.04) a) in units of angstroms, b) in km s -1, c) in km s -1 channel -1 Doppler Effect Iso-velocity contours in our Galaxy Rotation curve of our Galaxy (also from Bland & Blitz ) The kinematics of SNRs is a powerful tool that we can use to estimate the DISTANCE, and other important parameters of those objects. The Galactic SNR CTB 109 and the quest for its distance: Radio Einstein X-rays continuum, and CO CO and HI From Gregory & Falman (1980), Tatematsu et al. (1987), Kothes et al. (2002, 2006) While in the optical: Hurford & Fesen (1995) Sánchez -Cruces et al. (2017) 2D [SII]/Hα line-ratios of the optical filaments è a radiative shock Typical [SII] velocity profiles of two regions: è SNR CTB 109 IS IN THE PERSEUS ARM è THIS SNR HOSTING A MAGNETAR HAS RATHER TYPICAL INITIAL ENERGY II. -
A New Magnetic White Dwarf: PG 2329+267
Mon. Not. R. Astron. Soc. 299, 218–222 (1998) A new magnetic white dwarf: PG 2329+267 C. Moran,1 T. R. Marsh1 and V. S. Dhillon2 1University of Southampton, Department of Physics, Highfield, Southampton SO17 1BJ 2University of Sheffield, Department of Physics, Hounsfield Road, Sheffield S3 7RH Accepted 1998 April 27. Received 1998 April 3; in original form 1997 December 15 ABSTRACT We have discovered that the white dwarf PG 2329+267 is magnetic, and, assuming a centred dipole structure, has a dipole magnetic field strength of approximately 2.3 MG. This makes it one of only approximately 4 per cent of isolated white dwarfs with a detectable magnetic field. Linear Zeeman splitting, as well as quadratic Zeeman shifts, is evident in the hydrogen Balmer sequence and circular spectropolarimetry reveals ,10 per cent circular polarization in the two displaced j components of Ha. We suggest from comparison with spectra of white dwarfs of known mass that PG 2329+267 is more massive than typical isolated white dwarfs, in agreement with the hypothesis that magnetic white dwarfs evolve from magnetic chemically peculiar Ap and Bp type main-sequence stars. Key words: magnetic fields – polarization – stars: individual: PG 2329+267 – white dwarfs. remnants of magnetic main-sequence stars (Sion et al. 1988), as 1 INTRODUCTION well as the observed tendency for magnetic white dwarfs to be more The possibility that white dwarfs may possess large magnetic fields massive than non-magnetic white dwarfs because of their proposed was first suggested in 1947 (Blackett 1947); however, it was not evolution from more massive progenitors. -
Feedback by Massive Stars and the Emergence of Superbubbles
Astronomy & Astrophysics manuscript no. krause+2013_ESB_II_v10 c ESO 2018 January 3, 2018 Feedback by massive stars and the emergence of superbubbles II. X-ray properties Martin Krause1, 2,⋆, Roland Diehl1, 2, Hans Böhringer1, 2, Michael Freyberg1, and Daniel Lubos1 1 Max-Planck-Institut für extraterrestrische Physik, Giessenbachstr. 1, 85741 Garching, Germany 2 Excellence Cluster Universe, Technische Universität München, Boltzmannstrasse 2, 85748 Garching, Germany Received March 24, 2014; accepted ? ABSTRACT Context. In a previous paper we investigated the energy transfer of massive stars to the interstellar medium as a function of time and the geometrical configuration of three massive stars via 3D-mesh-refining hydrodynamics simulations, following the complete evolution of the massive stars and their supernovae except non-thermal processes . Aims. In order to compare our results against observations we derive thermal X-ray properties of the interstellar medium from our simulations and compare them to observations of superbubbles in general, to the well-studied nearby Orion-Eridanus superbubble and to the diffuse soft X-ray emission of nearby galaxies. Methods. We analysed our ISM simulation results with the help of spectra for plasma temperatures between 0.1 and 10 keV and computed the spectral evolution and the spatio-temporal distribution of the hot gas. Results. Despite significant input of high temperature gas from supernovae and fast stellar winds, the resulting thermal X-ray spectra are generally very soft, with most of the emission well below 1 keV. We show that this is due to mixing triggered by resolved hydrodynamic instabilities. Supernovae enhance the X-ray luminosity of a superbubble by 1-2 orders of magnitude for a time span of about 0.1 Myr; longer if a supernova occurs in a larger superbubble and shorter in higher energy bands. -
Lecture 17: the Solar Wind O Topics to Be Covered
Lecture 17: The solar wind o Topics to be covered: o Solar wind o Inteplanetary magnetic field The solar wind o Biermann (1951) noticed that many comets showed excess ionization and abrupt changes in the outflow of material in their tails - is this due to a solar wind? o Assumed comet orbit perpendicular to line-of-sight (vperp) and tail at angle ! => tan! = vperp/vr o From observations, tan ! ~ 0.074 o But vperp is a projection of vorbit -1 => vperp = vorbit sin ! ~ 33 km s -1 o From 600 comets, vr ~ 450 km s . o See Uni. New Hampshire course (Physics 954) for further details: http://www-ssg.sr.unh.edu/Physics954/Syllabus.html The solar wind o STEREO satellite image sequences of comet tail buffeting and disconnection. Parker’s solar wind o Parker (1958) assumed that the outflow from the Sun is steady, spherically symmetric and isothermal. o As PSun>>PISM => must drive a flow. o Chapman (1957) considered corona to be in hydrostatic equibrium: dP = −ρg dr dP GMS ρ + 2 = 0 Eqn. 1 dr r o If first term >> than second €=> produces an outflow: € dP GM ρ dv + S + ρ = 0 Eqn. 2 dr r2 dt o This is the equation for a steadily expanding solar/stellar wind. € Parker’s solar wind (cont.) dv dv dr dv dP GM ρ dv o As, = = v => + S + ρv = 0 dt dr dt dr dr r2 dr dv 1 dP GM or v + + S = 0 Eqn. 3 dr ρ dr r2 € € o Called the momentum equation. € o Eqn. 3 describes acceleration (1st term) of the gas due to a pressure gradient (2nd term) and gravity (3rd term).