The Inter-Eruption Timescale of Classical Novae from Expansion of the Z Camelopardalis Shell
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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. -
Z Cam Stars in the Twenty-First Century
Simonsen et al., JAAVSO Volume 42, 2014 1 Z Cam Stars in the Twenty-First Century Mike Simonsen AAVSO, 49 Bay State Road., Cambridge, MA 02138; [email protected] David Boyd 5 Silver Lane, West Challow OX12 9TX, England; [email protected] William Goff 13508 Monitor Lane, Sutter Creek, CA 95685; [email protected] Tom Krajci Center for Backyard Astronomy, P.O. Box 1351, Cloudcroft, NM 88317; [email protected] Kenneth Menzies 318A Potter Road, Framingham MA, 01701; [email protected] Sebastian Otero AAVSO, 49 Bay State Road, Cambridge, MA 02138; [email protected] Stefano Padovan Barrio Masos SN, 17132 Foixà, Girona, Spain; [email protected] Gary Poyner 67 Ellerton Road, Kingstanding, Birmingham B44 0QE, England; [email protected] James Roe 85 Eikermann Road-174, Bourbon, MO 65441; [email protected] Richard Sabo 2336 Trailcrest Drive, Bozeman, MT 59718; [email protected] George Sjoberg 9 Contentment Crest, #182, Mayhill, NM 88339; [email protected] Bart Staels Koningshofbaan 51, Hofstade (Aalst) B-9308, Belgium; [email protected] Rod Stubbings 2643 Warragul, Korumburra Road, Tetoora Road, VIC 3821, Australia; [email protected] John Toone 17 Ashdale Road, Cressage, Shrewsbury SY5 6DT, England; [email protected] Patrick Wils Aarschotsebaan 31, Hever B-3191, Belgium; [email protected] Received October 7, 2013; revised November 12, 2013; accepted November 12, 2013 2 Simonsen et al., JAAVSO Volume 42, 2014 Abstract Z Cam (UGZ) stars are a small subset of dwarf novae that exhibit standstills in their light curves. Most modern literature and catalogs of cataclysmic variables quote the number of known Z Cams to be on the order of thirty or so systems. -
Variable Star Classification and Light Curves Manual
Variable Star Classification and Light Curves An AAVSO course for the Carolyn Hurless Online Institute for Continuing Education in Astronomy (CHOICE) This is copyrighted material meant only for official enrollees in this online course. Do not share this document with others. Please do not quote from it without prior permission from the AAVSO. Table of Contents Course Description and Requirements for Completion Chapter One- 1. Introduction . What are variable stars? . The first known variable stars 2. Variable Star Names . Constellation names . Greek letters (Bayer letters) . GCVS naming scheme . Other naming conventions . Naming variable star types 3. The Main Types of variability Extrinsic . Eclipsing . Rotating . Microlensing Intrinsic . Pulsating . Eruptive . Cataclysmic . X-Ray 4. The Variability Tree Chapter Two- 1. Rotating Variables . The Sun . BY Dra stars . RS CVn stars . Rotating ellipsoidal variables 2. Eclipsing Variables . EA . EB . EW . EP . Roche Lobes 1 Chapter Three- 1. Pulsating Variables . Classical Cepheids . Type II Cepheids . RV Tau stars . Delta Sct stars . RR Lyr stars . Miras . Semi-regular stars 2. Eruptive Variables . Young Stellar Objects . T Tau stars . FUOrs . EXOrs . UXOrs . UV Cet stars . Gamma Cas stars . S Dor stars . R CrB stars Chapter Four- 1. Cataclysmic Variables . Dwarf Novae . Novae . Recurrent Novae . Magnetic CVs . Symbiotic Variables . Supernovae 2. Other Variables . Gamma-Ray Bursters . Active Galactic Nuclei 2 Course Description and Requirements for Completion This course is an overview of the types of variable stars most commonly observed by AAVSO observers. We discuss the physical processes behind what makes each type variable and how this is demonstrated in their light curves. Variable star names and nomenclature are placed in a historical context to aid in understanding today’s classification scheme. -
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. -
Rapid Oscillations in Cataclysmic Variables
I RAPID OSCILLATIONS IN CATACLYSMIC VARIABLES Sue Allen . ' Thesis submitted for the degree of l Master of Science at the University of Cape Town July 1986 'I.-~~,,,.,------.. The Unlvers{ty bf qape Town tias been given the right to reproduce t~!s thesis in whole or in part. Copytlght Is hehl ~y the author. The copyright of this thesis vests in the author. No quotation from it or information derived from it is to be published without full acknowledgement of the source. The thesis is to be used for private study or non- commercial research purposes only. Published by the University of Cape Town (UCT) in terms of the non-exclusive license granted to UCT by the author. ACKNOWLEDGEMENTS I am indebted to my supervisor, Professor B. Warner, for his guidance and patience and for securing me financial support for this work. I am·· grateful to the Director of the south African Astronomical Observatory, Dr M. Feast, for the allocation of observing time and for' allowing me to use the Observatory Library over an extended period .. Thanks also to Mrs E:. Lastovica and Dr L. Balona, and especially to Drs o. Kilkenny and I. Coulson for constant encouragement and for putting up with a "squatter" in their office. Dr o. O'Donoghue wrote all the computer programs used in the data analysis, and gave me great moral support and much of his time. My thanks go to Mrs P. Debbie and Mrs c. Barends for help with the worst of the typing, and to Dr I. Coulson for proofreading the manuscript. -
A New Review of Old Novae
Acta Polytechnica CTU Proceedings 2(1): 199{204, 2015 doi: 10.14311/APP.2015.02.0199 199 199 A New Review of Old Novae A. Pagnotta1 1American Museum of Natural History Corresponding author: [email protected] Abstract Novae are certainly very exciting at the time of their eruptions, and there is much work left to be done in understanding all of the details of that part of their existence, but there is also much to be learned by looking at the systems decades, centuries, and even millennia after their peak. I give a brief overview of some of the history and motivation behind studying old novae and long-term nova evolution, and then focus on the state of the field today. Exciting new results are finally starting to shed some light on the secular behavior of post-nova systems, although as is often the case in astronomy, the observations are at times conflicting. As is always the case, we need more observations and better theoretical frameworks to truly understand the situation. Keywords: novae - dwarf novae - cataclysmic variables - photometry. 1 Introduction were quantified into the hibernation model originally proposed by Shara et al. (1986) to explain the low ob- Novae have been observed at least as far back as 134 served space-density of novae. Although more recent B.C. (Fontanille 2007), and we continue to observe surveys seem to show that the low numbers of observed them and their kin|recurrent novae (RNe), dwarf no- novae at the time may have been due to observational vae (DNe), and the rest of the cataclysmic variables limitations and biases, (e.g. -
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). -
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. -
Astronomy General Information
ASTRONOMY GENERAL INFORMATION HERTZSPRUNG-RUSSELL (H-R) DIAGRAMS -A scatter graph of stars showing the relationship between the stars’ absolute magnitude or luminosities versus their spectral types or classifications and effective temperatures. -Can be used to measure distance to a star cluster by comparing apparent magnitude of stars with abs. magnitudes of stars with known distances (AKA model stars). Observed group plotted and then overlapped via shift in vertical direction. Difference in magnitude bridge equals distance modulus. Known as Spectroscopic Parallax. SPECTRA HARVARD SPECTRAL CLASSIFICATION (1-D) -Groups stars by surface atmospheric temp. Used in H-R diag. vs. Luminosity/Abs. Mag. Class* Color Descr. Actual Color Mass (M☉) Radius(R☉) Lumin.(L☉) O Blue Blue B Blue-white Deep B-W 2.1-16 1.8-6.6 25-30,000 A White Blue-white 1.4-2.1 1.4-1.8 5-25 F Yellow-white White 1.04-1.4 1.15-1.4 1.5-5 G Yellow Yellowish-W 0.8-1.04 0.96-1.15 0.6-1.5 K Orange Pale Y-O 0.45-0.8 0.7-0.96 0.08-0.6 M Red Lt. Orange-Red 0.08-0.45 *Very weak stars of classes L, T, and Y are not included. -Classes are further divided by Arabic numerals (0-9), and then even further by half subtypes. The lower the number, the hotter (e.g. A0 is hotter than an A7 star) YERKES/MK SPECTRAL CLASSIFICATION (2-D!) -Groups stars based on both temperature and luminosity based on spectral lines.