Cataclysmic Variables from USNO-B1.0 Catalog: Stars with Outbursts on Infrared Palomar Plates
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White Dwarfs and Electron Degeneracy
White Dwarfs and Electron Degeneracy Farley V. Ferrante Southern Methodist University Sirius A and B 27 March 2017 SMU PHYSICS 1 Outline • Stellar astrophysics • White dwarfs • Dwarf novae • Classical novae • Supernovae • Neutron stars 27 March 2017 SMU PHYSICS 2 27 March 2017 SMU PHYSICS 3 Pogson’s ratio: 5 100≈ 2.512 27 March 2017 M.S. Physics Thesis Presentation 4 Distance Modulus mM−=5 log10 ( d) − 1 • Absolute magnitude (M) • Apparent magnitude of an object at a standard luminosity distance of exactly 10.0 parsecs (~32.6 ly) from the observer on Earth • Allows true luminosity of astronomical objects to be compared without regard to their distances • Unit: parsec (pc) • Distance at which 1 AU subtends an angle of 1″ • 1 AU = 149 597 870 700 m (≈1.50 x 108 km) • 1 pc ≈ 3.26 ly • 1 pc ≈ 206 265 AU 27 March 2017 SMU PHYSICS 5 Stellar Astrophysics • Stefan-Boltzmann Law: 54 2π k − − −− FT=σσ4; = = 5.67x 10 5 ergs 1 cm 24 K bol 15ch23 • Effective temperature of a star: Temp. of a black body with the same luminosity per surface area • Stars can be treated as black body radiators to a good approximation • Effective surface temperature can be obtained from the B-V color index with the Ballesteros equation: 11 T = 4600+ 0.92(BV−+) 1.70 0.92(BV −+) 0.62 • Luminosity: 24 L= 4πσ rT* E 27 March 2017 SMU PHYSICS 6 H-R Diagram 27 March 2017 SMU PHYSICS 8 27 March 2017 SMU PHYSICS 9 White dwarf • Core of solar mass star • Pauli exclusion principle: Electron degeneracy • Degenerate Fermi gas of oxygen and carbon • 1 teaspoon would weigh 5 tons • No energy produced from fusion or gravitational contraction Hot white dwarf NGC 2440. -
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. -
Mira Variables: an Informal Review
MIRA VARIABLES: AN INFORMAL REVIEW ROBERT F. WING Astronomy Department, Ohio State University The Mira variables can be either fascinating or frustrating -- depending on whether one is content to watch them go through their changes or whether one insists on understanding them. Virtually every observable property of the Miras, including each detail of their extraordinarily complex spectra, is strongly time-dependent. Most of the changes are cyclic with a period equal to that of the light variation. It is well known, however, that the lengths of individual light cycles often differ noticeably from the star's mean period, the differences typically amounting to several percent. And if you observe Miras -- no matter what kind of observation you make -- your work is never done, because none of their observable properties repeats exactly from cycle to cycle. The structure of Mira variables can perhaps best be described as loose. They are enormous, distended stars, and it is clear that many differ- ent atmospheric layers contribute to the spectra (and photometric colors) that we observe. As we shall see, these layers can have greatly differing temperatures, and the cyclical temperature variations of the various layers are to some extent independent of one another. Here no doubt is the source of many of the apparent inconsistencies in the observational data, as well as the phase lags between light curves in different colors. But when speaking of "layers" in the atmosphere, we should remember that they merge into one another, and that layers that are spectroscopically distinct by virtue of thelrvertical motions may in fact be momentarily at the same height in the atmosphere. -
The Inter-Eruption Timescale of Classical Novae from Expansion of the Z Camelopardalis Shell
The Astrophysical Journal, 756:107 (6pp), 2012 September 10 doi:10.1088/0004-637X/756/2/107 C 2012. The American Astronomical Society. All rights reserved. Printed in the U.S.A. THE INTER-ERUPTION TIMESCALE OF CLASSICAL NOVAE FROM EXPANSION OF THE Z CAMELOPARDALIS SHELL Michael M. Shara1,4, Trisha Mizusawa1, David Zurek1,4, Christopher D. Martin2, James D. Neill2, and Mark Seibert3 1 Department of Astrophysics, American Museum of Natural History, Central Park West at 79th Street, New York, NY 10024-5192, USA 2 Department of Physics, Math and Astronomy, California Institute of Technology, 1200 East California Boulevard, Mail Code 405-47, Pasadena, CA 91125, USA 3 Observatories of the Carnegie Institution of Washington, 813 Santa Barbara Street, Pasadena, CA 91101, USA Received 2012 May 14; accepted 2012 July 9; published 2012 August 21 ABSTRACT The dwarf nova Z Camelopardalis is surrounded by the largest known classical nova shell. This shell demonstrates that at least some dwarf novae must have undergone classical nova eruptions in the past, and that at least some classical novae become dwarf novae long after their nova thermonuclear outbursts. The current size of the shell, its known distance, and the largest observed nova ejection velocity set a lower limit to the time since Z Cam’s last outburst of 220 years. The radius of the brightest part of Z Cam’s shell is currently ∼880 arcsec. No expansion of the radius of the brightest part of the ejecta was detected, with an upper limit of 0.17 arcsec yr−1. This suggests that the last Z Cam eruption occurred 5000 years ago. -
AT Cnc: a SECOND DWARF NOVA with a CLASSICAL NOVA SHELL
The Astrophysical Journal, 758:121 (5pp), 2012 October 20 doi:10.1088/0004-637X/758/2/121 C 2012. The American Astronomical Society. All rights reserved. Printed in the U.S.A. AT Cnc: A SECOND DWARF NOVA WITH A CLASSICAL NOVA SHELL Michael M. Shara1,5, Trisha Mizusawa1, Peter Wehinger2, David Zurek1,5,6, Christopher D. Martin3, James D. Neill3, Karl Forster3, and Mark Seibert4 1 Department of Astrophysics, American Museum of Natural History, Central Park West at 79th Street, New York, NY 10024-5192, USA 2 Steward Observatory, the University of Arizona, 933 North Cherry Avenue, Tucson, AZ 85721, USA 3 Department of Physics, Math and Astronomy, California Institute of Technology, 1200 East California Boulevard, Mail Code 405-47, Pasadena, CA 91125, USA 4 Observatories of the Carnegie Institution of Washington, 813 Santa Barbara Street, Pasadena, CA 91101, USA Received 2012 July 31; accepted 2012 August 23; published 2012 October 8 ABSTRACT We are systematically surveying all known and suspected Z Cam-type dwarf novae for classical nova shells. This survey is motivated by the discovery of the largest known classical nova shell, which surrounds the archetypal dwarf nova Z Camelopardalis. The Z Cam shell demonstrates that at least some dwarf novae must have undergone classical nova eruptions in the past, and that at least some classical novae become dwarf novae long after their nova thermonuclear outbursts, in accord with the hibernation scenario of cataclysmic binaries. Here we report the detection of a fragmented “shell,” 3 arcmin in diameter, surrounding the dwarf nova AT Cancri. This second discovery demonstrates that nova shells surrounding Z Cam-type dwarf novae cannot be very rare. -
A Review of the Disc Instability Model for Dwarf Novae, Soft X-Ray Transients and Related Objects a J.M
A review of the disc instability model for dwarf novae, soft X-ray transients and related objects a J.M. Hameury aObservatoire Astronomique de Strasbourg ARTICLEINFO ABSTRACT Keywords: I review the basics of the disc instability model (DIM) for dwarf novae and soft-X-ray transients Cataclysmic variable and its most recent developments, as well as the current limitations of the model, focusing on the Accretion discs dwarf nova case. Although the DIM uses the Shakura-Sunyaev prescription for angular momentum X-ray binaries transport, which we know now to be at best inaccurate, it is surprisingly efficient in reproducing the outbursts of dwarf novae and soft X-ray transients, provided that some ingredients, such as irradiation of the accretion disc and of the donor star, mass transfer variations, truncation of the inner disc, etc., are added to the basic model. As recently realized, taking into account the existence of winds and outflows and of the torque they exert on the accretion disc may significantly impact the model. I also discuss the origin of the superoutbursts that are probably due to a combination of variations of the mass transfer rate and of a tidal instability. I finally mention a number of unsolved problems and caveats, among which the most embarrassing one is the modelling of the low state. Despite significant progresses in the past few years both on our understanding of angular momentum transport, the DIM is still needed for understanding transient systems. 1. Introduction tems using Doppler tomography techniques (Steeghs et al. 1997; Marsh and Horne 1988; see also Marsh and Schwope Dwarf novae (DNe) are cataclysmic variables (CV) that 2016 for a recent review). -
(NASA/Chandra X-Ray Image) Type Ia Supernova Remnant – Thermonuclear Explosion of a White Dwarf
Stellar Evolution Card Set Description and Links 1. Tycho’s SNR (NASA/Chandra X-ray image) Type Ia supernova remnant – thermonuclear explosion of a white dwarf http://chandra.harvard.edu/photo/2011/tycho2/ 2. Protostar formation (NASA/JPL/Caltech/Spitzer/R. Hurt illustration) A young star/protostar forming within a cloud of gas and dust http://www.spitzer.caltech.edu/images/1852-ssc2007-14d-Planet-Forming-Disk- Around-a-Baby-Star 3. The Crab Nebula (NASA/Chandra X-ray/Hubble optical/Spitzer IR composite image) A type II supernova remnant with a millisecond pulsar stellar core http://chandra.harvard.edu/photo/2009/crab/ 4. Cygnus X-1 (NASA/Chandra/M Weiss illustration) A stellar mass black hole in an X-ray binary system with a main sequence companion star http://chandra.harvard.edu/photo/2011/cygx1/ 5. White dwarf with red giant companion star (ESO/M. Kornmesser illustration/video) A white dwarf accreting material from a red giant companion could result in a Type Ia supernova http://www.eso.org/public/videos/eso0943b/ 6. Eight Burst Nebula (NASA/Hubble optical image) A planetary nebula with a white dwarf and companion star binary system in its center http://apod.nasa.gov/apod/ap150607.html 7. The Carina Nebula star-formation complex (NASA/Hubble optical image) A massive and active star formation region with newly forming protostars and stars http://www.spacetelescope.org/images/heic0707b/ 8. NGC 6826 (Chandra X-ray/Hubble optical composite image) A planetary nebula with a white dwarf stellar core in its center http://chandra.harvard.edu/photo/2012/pne/ 9. -
Stellar Evolution
AccessScience from McGraw-Hill Education Page 1 of 19 www.accessscience.com Stellar evolution Contributed by: James B. Kaler Publication year: 2014 The large-scale, systematic, and irreversible changes over time of the structure and composition of a star. Types of stars Dozens of different types of stars populate the Milky Way Galaxy. The most common are main-sequence dwarfs like the Sun that fuse hydrogen into helium within their cores (the core of the Sun occupies about half its mass). Dwarfs run the full gamut of stellar masses, from perhaps as much as 200 solar masses (200 M,⊙) down to the minimum of 0.075 solar mass (beneath which the full proton-proton chain does not operate). They occupy the spectral sequence from class O (maximum effective temperature nearly 50,000 K or 90,000◦F, maximum luminosity 5 × 10,6 solar), through classes B, A, F, G, K, and M, to the new class L (2400 K or 3860◦F and under, typical luminosity below 10,−4 solar). Within the main sequence, they break into two broad groups, those under 1.3 solar masses (class F5), whose luminosities derive from the proton-proton chain, and higher-mass stars that are supported principally by the carbon cycle. Below the end of the main sequence (masses less than 0.075 M,⊙) lie the brown dwarfs that occupy half of class L and all of class T (the latter under 1400 K or 2060◦F). These shine both from gravitational energy and from fusion of their natural deuterium. Their low-mass limit is unknown. -
Spectroscopy and Orbital Periods of Four Cataclysmic Variable Stars
Dartmouth College Dartmouth Digital Commons Open Dartmouth: Published works by Dartmouth faculty Faculty Work 10-1-2001 Spectroscopy and Orbital Periods of Four Cataclysmic Variable Stars John R. Thorstensen Dartmouth College Cynthia J. Taylor Dartmouth College Follow this and additional works at: https://digitalcommons.dartmouth.edu/facoa Part of the Stars, Interstellar Medium and the Galaxy Commons Dartmouth Digital Commons Citation Thorstensen, John R. and Taylor, Cynthia J., "Spectroscopy and Orbital Periods of Four Cataclysmic Variable Stars" (2001). Open Dartmouth: Published works by Dartmouth faculty. 1868. https://digitalcommons.dartmouth.edu/facoa/1868 This Article is brought to you for free and open access by the Faculty Work at Dartmouth Digital Commons. It has been accepted for inclusion in Open Dartmouth: Published works by Dartmouth faculty by an authorized administrator of Dartmouth Digital Commons. For more information, please contact [email protected]. Mon. Not. R. Astron. Soc. 326, 1235–1242 (2001) Spectroscopy and orbital periods of four cataclysmic variable stars John R. ThorstensenP and Cynthia J. Taylor Department of Physics and Astronomy, Dartmouth College, Hanover, NH 03755, USA Accepted 2001 May 2. Received 2001 May 2; in original form 2001 March 29 ABSTRACT We present spectroscopy and orbital periods Porb of four relatively little-studied cataclysmic variable stars. The stars and their periods are: AF Cam, Porb ¼ 0:324ð1Þ d (the daily cycle count is slightly ambiguous); V2069 Cyg (¼ RX J2123.714217), 0.311683(2) d; PG 09351075, 0.1868(3) d; and KUV 0358010614, 0.1495(6) d. V2069 Cyg and KUV 0358010614 both show He II l4686 emission comparable in strength to Hb. -
Cosmic Catastrophes Wheeler 309N Spring 2008 April 7, 2008 (49490) Review for Test #3 Neutron Stars and Black Holes
Cosmic Catastrophes Wheeler 309N Spring 2008 April 7, 2008 (49490) Review for Test #3 Neutron Stars and Black Holes Neutron stars – mass of sun, radius ~ 10km, density like atomic nucleus, huge gravity at surface. Discovery of pulsars – pulsating radio sources Interpretation of pulsars as rotating magnetized neutron stars Role of magnetic field to cause radiation, misalignment of rotation axis, magnetic axis Production of pulses – probably related to strong electric, magnetic fields at magnetic poles About 600 pulsars known, perhaps a billion neutron stars in the Galaxy. Pressure support from quantum pressure of neutrons plus nuclear repulsion. Maximum mass of neutron star about 2 solar masses. Neutron stars as binary X-rays sources. X-ray pulsars – accreted gas channeled to magnetic poles, “pulsar” by lighthouse effect if magnetic axis is tilted with respect to the spin axis. X-ray transients – 4 or 5 known in our Galaxy. Outburst every few years for a month. Probably a disk instability like a dwarf nova, but with the white dwarf replaced by a neutron star. X-ray Bursters – about 30 known in our Galaxy. Burst every few hours for minutes. Probably the neutron star analog of a classical nova. Matter accretes on surface of neutron star. Hydrogen is supported by thermal pressure, burns to helium. Helium is supported by quantum pressure and is unregulated and explodes, producing the X-rays. Magnetars – neutron stars with magnetic fields 100 to 1000 times stronger than the Crab nebula pulsar. Soft gamm-ray repeaters – objects that emit intense bursts of low energy gamma rays and X-rays for a few minutes every few years. -
Cataclysmic Variables
Cataclysmic variables Article (Accepted Version) Smith, Robert Connon (2006) Cataclysmic variables. Contemporary Physics, 47 (6). pp. 363-386. ISSN 0010-7514 This version is available from Sussex Research Online: http://sro.sussex.ac.uk/id/eprint/2256/ This document is made available in accordance with publisher policies and may differ from the published version or from the version of record. If you wish to cite this item you are advised to consult the publisher’s version. Please see the URL above for details on accessing the published version. Copyright and reuse: Sussex Research Online is a digital repository of the research output of the University. Copyright and all moral rights to the version of the paper presented here belong to the individual author(s) and/or other copyright owners. To the extent reasonable and practicable, the material made available in SRO has been checked for eligibility before being made available. Copies of full text items generally can be reproduced, displayed or performed and given to third parties in any format or medium for personal research or study, educational, or not-for-profit purposes without prior permission or charge, provided that the authors, title and full bibliographic details are credited, a hyperlink and/or URL is given for the original metadata page and the content is not changed in any way. http://sro.sussex.ac.uk Cataclysmic variables Robert Connon Smith Department of Physics and Astronomy, University of Sussex, Falmer, Brighton BN1 9QH, UK E-mail: [email protected] Abstract. Cataclysmic variables are binary stars in which a relatively normal star is transferring mass to its compact companion. -
Variable Star
Variable star A variable star is a star whose brightness as seen from Earth (its apparent magnitude) fluctuates. This variation may be caused by a change in emitted light or by something partly blocking the light, so variable stars are classified as either: Intrinsic variables, whose luminosity actually changes; for example, because the star periodically swells and shrinks. Extrinsic variables, whose apparent changes in brightness are due to changes in the amount of their light that can reach Earth; for example, because the star has an orbiting companion that sometimes Trifid Nebula contains Cepheid variable stars eclipses it. Many, possibly most, stars have at least some variation in luminosity: the energy output of our Sun, for example, varies by about 0.1% over an 11-year solar cycle.[1] Contents Discovery Detecting variability Variable star observations Interpretation of observations Nomenclature Classification Intrinsic variable stars Pulsating variable stars Eruptive variable stars Cataclysmic or explosive variable stars Extrinsic variable stars Rotating variable stars Eclipsing binaries Planetary transits See also References External links Discovery An ancient Egyptian calendar of lucky and unlucky days composed some 3,200 years ago may be the oldest preserved historical document of the discovery of a variable star, the eclipsing binary Algol.[2][3][4] Of the modern astronomers, the first variable star was identified in 1638 when Johannes Holwarda noticed that Omicron Ceti (later named Mira) pulsated in a cycle taking 11 months; the star had previously been described as a nova by David Fabricius in 1596. This discovery, combined with supernovae observed in 1572 and 1604, proved that the starry sky was not eternally invariable as Aristotle and other ancient philosophers had taught.