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145, September 2010
British Astronomical Association VARIABLE STAR SECTION CIRCULAR No 145, September 2010 Contents EG Andromedae Light Curve ................................................... inside front cover From the Director ............................................................................................... 1 Letter Page. Visual Observing ............................................................................ 4 Epsilon Aurigae Spectroscopically at Mid Eclipse .......................................... 5 Eclipsing Binary News ...................................................................................... 7 AO Cassiopeiae Phase Diagram ............................................................ 9 PV Cephei and Gyulbudaghian’s Nebula ........................................................ 10 WR140 Periastron Campaign Update .............................................................. 12 VSS Meeting, Pendrell Hall. The Central Stars of Planetary Nebulae ............ 14 RR Coronae Borealis 1993-2004 ...................................................................... 16 TU Cassiopeiae Phase Diagram 2005-2010 ..................................................... 18 Binocular Priority List ..................................................................................... 19 Eclipsing Binary Predictions ............................................................................ 20 Charges for Section Publications .............................................. inside back cover Guidelines for Contributing to the Circular ............................. -
Alyssa Goodman, Naomi Ridge, Scott Wolk, Scott Schnee, Di Li & Bryan
COMPLET(E)ING THE STAR-FORMATION HISTORY OF THE RHO-OPH REGION Alyssa Goodman, Naomi Ridge, Scott Wolk, Scott Schnee, Di Li & Bryan Gaensler Background The interaction of newly formed stars with their parent cloud, particularly in the case of massive stars, can have significant consequences for the subsequent development of the cloud. Hot, massive stars will cause cloud disruption through their ionizing flux as well as through the momentum in their stellar winds. Alternatively, given the right conditions in the cloud, stellar winds may also cause the collapse of cloud cores and induce further star formation. Located only 160pc from the Sun, the Ophiuchus molecular cloud is one of the most conspicuous nearby regions where low- and intermediate-mass star formation is taking place (e.g. Wilking 1992 for a review). The Ophiuchus cloud consists of two massive, centrally condensed cores, L1688 and L1689, from each of which a filamentary system of streamers extends to the north-east over tens of parsecs (e.g. Loren 1989). While little star formation activity is observed in the streamers, the westernmost core, L1688 (figure 1), harbors a rich cluster of young stellar objects (YSOs) at various evolutionary stages and is distinguished by a high star-formation efficiency (Wilking & Lada 1983 - hereafter WL83). This young stellar cluster and the cloud core in which it resides are commonly referred to as the ρ-Oph star-forming region. Both the gas/dust content and the embedded stellar population of ρ−Oph have been extensively studied for more than two decades. The distribution of the low-density molecular gas was mapped in C18O(1-0) by WL83, revealing a ridge of high column density gas. -
The Impact of the Astro2010 Recommendations on Variable Star Science
The Impact of the Astro2010 Recommendations on Variable Star Science Corresponding Authors Lucianne M. Walkowicz Department of Astronomy, University of California Berkeley [email protected] phone: (510) 642–6931 Andrew C. Becker Department of Astronomy, University of Washington [email protected] phone: (206) 685–0542 Authors Scott F. Anderson, Department of Astronomy, University of Washington Joshua S. Bloom, Department of Astronomy, University of California Berkeley Leonid Georgiev, Universidad Autonoma de Mexico Josh Grindlay, Harvard–Smithsonian Center for Astrophysics Steve Howell, National Optical Astronomy Observatory Knox Long, Space Telescope Science Institute Anjum Mukadam, Department of Astronomy, University of Washington Andrej Prsa,ˇ Villanova University Joshua Pepper, Villanova University Arne Rau, California Institute of Technology Branimir Sesar, Department of Astronomy, University of Washington Nicole Silvestri, Department of Astronomy, University of Washington Nathan Smith, Department of Astronomy, University of California Berkeley Keivan Stassun, Vanderbilt University Paula Szkody, Department of Astronomy, University of Washington Science Frontier Panels: Stars and Stellar Evolution (SSE) February 16, 2009 Abstract The next decade of survey astronomy has the potential to transform our knowledge of variable stars. Stellar variability underpins our knowledge of the cosmological distance ladder, and provides direct tests of stellar formation and evolution theory. Variable stars can also be used to probe the fundamental physics of gravity and degenerate material in ways that are otherwise impossible in the laboratory. The computational and engineering advances of the past decade have made large–scale, time–domain surveys an immediate reality. Some surveys proposed for the next decade promise to gather more data than in the prior cumulative history of astronomy. -
Distances and Magnitudes Distance Measurements the Cosmic Distance
Distances and Magnitudes Prof Andy Lawrence Astronomy 1G 2011-12 Distance Measurements Astronomy 1G 2011-12 The cosmic distance ladder • Distance measurements in astronomy are a chain, with each type of measurement relative to the one before • The bottom rung is the Astronomical Unit (AU), the (mean) distance between the Earth and the Sun • Many distance estimates rely on the idea of a "standard candle" or "standard yardstick" Astronomy 1G 2011-12 Distances in the solar system • relative distances to planets given by periods + Keplers law (see Lecture-2) • distance to Venus measured by radar • Sun-Earth = 1 A.U. (average) • Sun-Jupiter = 5 A.U. (average) • Sun-Neptune = 30 A.U. (average) • Sun- Oort cloud (comets) ~ 50,000 A.U. • 1 A.U. = 1.496 x 1011 m Astronomy 1G 2011-12 Distances to nearest stars • parallax against more distant non- moving stars • 1 parsec (pc) is defined as distance where parallax = 1 second of arc in standard units D = a/✓ (radians, metres) in AU and arcsec D(AU) = 1/✓rad = 206, 265/✓00 in parsec and arcsec D(pc) = 1/✓00 nearest star Proxima Centauri 1.30pc Very hard to measure less than 0.1" 1pc = 206,265 AU = 3.086 x 1016m so only good for stars a few parsecs away... until launch of GAIA mission in 2014..... Astronomy 1G 2011-12 More distant stars : standard candle technique If a star has luminosity L (total energy emitted per sec) then at L distance D we will observe flux density F (i.e. energy per second F = 2 per sq.m. -
Standard Candles in Cosmology
Standard Candles: Distance Measurement in Astronomy Farley V. Ferrante Southern Methodist University 5/3/2017 PHYS 3368: Principles of Astrophysics & Cosmology 1 OUTLINE • Cosmic Distance Ladder • Standard Candles Parallax Cepheid variables Planetary nebula Most luminous supergiants Most luminous globular clusters Most luminous H II regions Supernovae Hubble constant & red shift • Standard Model of Cosmology 5/3/2017 PHYS 3368: Principles of Astrophysics & Cosmology 2 The Cosmic Distance Ladder - Distances far too vast to be measured directly - Several methods of indirect measurement - Clever methods relying on careful observation and basic mathematics - Cosmic distance ladder: A progression of indirect methods which scale, overlap, & calibrate parameters for large distances in terms of smaller distances • More methods calibrate these distances until distances that can be measured directly are achieved 5/3/2017 PHYS 3368: Principles of Astrophysics & Cosmology 3 Standard Candles • Magnitude: Historical unit (Hipparchus) of stellar brightness such that 5 magnitudes represents a factor of 100 in intensity • Apparent magnitude: Number assigned to visual brightness of an object; originally a scale of 1-6 • Absolute magnitude: Magnitude an object would have at 10 pc (convenient distance for comparison) • List of most luminous stars 5/3/2017 PHYS 3368: Principles of Astrophysics & Cosmology 4 5/3/2017 PHYS 3368: Principles of Astrophysics & Cosmology 5 The Cosmic Distance Ladder 5/3/2017 PHYS 3368: Principles of Astrophysics & Cosmology 6 The -
A Basic Requirement for Studying the Heavens Is Determining Where In
Abasic requirement for studying the heavens is determining where in the sky things are. To specify sky positions, astronomers have developed several coordinate systems. Each uses a coordinate grid projected on to the celestial sphere, in analogy to the geographic coordinate system used on the surface of the Earth. The coordinate systems differ only in their choice of the fundamental plane, which divides the sky into two equal hemispheres along a great circle (the fundamental plane of the geographic system is the Earth's equator) . Each coordinate system is named for its choice of fundamental plane. The equatorial coordinate system is probably the most widely used celestial coordinate system. It is also the one most closely related to the geographic coordinate system, because they use the same fun damental plane and the same poles. The projection of the Earth's equator onto the celestial sphere is called the celestial equator. Similarly, projecting the geographic poles on to the celest ial sphere defines the north and south celestial poles. However, there is an important difference between the equatorial and geographic coordinate systems: the geographic system is fixed to the Earth; it rotates as the Earth does . The equatorial system is fixed to the stars, so it appears to rotate across the sky with the stars, but of course it's really the Earth rotating under the fixed sky. The latitudinal (latitude-like) angle of the equatorial system is called declination (Dec for short) . It measures the angle of an object above or below the celestial equator. The longitud inal angle is called the right ascension (RA for short). -
Nebula in NGC 2264
Durham E-Theses The polarisation of the cone(IRN) Nebula in NGC 2264 Hill, Marianne C.M. How to cite: Hill, Marianne C.M. (1991) The polarisation of the cone(IRN) Nebula in NGC 2264, Durham theses, Durham University. Available at Durham E-Theses Online: http://etheses.dur.ac.uk/6098/ Use policy The full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-prot purposes provided that: • a full bibliographic reference is made to the original source • a link is made to the metadata record in Durham E-Theses • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders. Please consult the full Durham E-Theses policy for further details. Academic Support Oce, Durham University, University Oce, Old Elvet, Durham DH1 3HP e-mail: [email protected] Tel: +44 0191 334 6107 http://etheses.dur.ac.uk THE POLARISATION OF THE CONE(IRN) NEBULA IN NGC 2264 MARIANNE C. M. HILL A Thesis submitted to the University of Durham for the degree of Master of Science. The copyright of this thesis rests with the author. No quotation from it should be published without prior consent and information derived from it should be acknowledged. Department of Physics. September 1991 The copyright of this thesis rests with the author. No quotation from it should be published without his prior written consent and information derived from it should be acknowledged. -
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Research Paper J. Astron. Space Sci. 31(3), 187-197 (2014) http://dx.doi.org/10.5140/JASS.2014.31.3.187 An Orbital Stability Study of the Proposed Companions of SW Lyncis T. C. Hinse1†, Jonathan Horner2,3, Robert A. Wittenmyer3,4 1Korea Astronomy and Space Science Institute, Daejeon 305-348, Korea 2Computational Engineering and Science Research Centre, University of Southern Queensland, Toowoomba, Queensland 4350, Australia 3Australian Centre for Astrobiology, University of New South Wales, Sydney 2052, Australia 4School of Physics, University of New South Wales, Sydney 2052, Australia We have investigated the dynamical stability of the proposed companions orbiting the Algol type short-period eclipsing binary SW Lyncis (Kim et al. 2010). The two candidate companions are of stellar to substellar nature, and were inferred from timing measurements of the system’s primary and secondary eclipses. We applied well-tested numerical techniques to accurately integrate the orbits of the two companions and to test for chaotic dynamical behavior. We carried out the stability analysis within a systematic parameter survey varying both the geometries and orientation of the orbits of the companions, as well as their masses. In all our numerical integrations we found that the proposed SW Lyn multi-body system is highly unstable on time-scales on the order of 1000 years. Our results cast doubt on the interpretation that the timing variations are caused by two companions. This work demonstrates that a straightforward dynamical analysis can help to test whether a best-fit companion-based model is a physically viable explanation for measured eclipse timing variations. -
The Ancient Star Catalog
Vol. 12 2002 Sept ISSN 10415440 DIO The International Journal of Scientific History The Ancient Star Catalog Novel Evidence at the Southern Limit (still) points to Hipparchan authorship Instruments & Coordinate Systems New Star Identifications 2 2002 Sept DIO 12 2002 Sept DIO 12 3 Table of Contents Page: 1 The Southern Limit of the Ancient Star Catalog by KEITH A. PICKERING 3 z z1 The Southern Limits of the Ancient Star Catalog 2 On the Clarity of Visibility Tests by DENNIS DUKE 28 z and the Commentary of Hipparchos 3 The Measurement Method of the Almagest Stars by DENNIS DUKE 35 z 4 The Instruments Used by Hipparchos by KEITH A. PICKERING 51 by KEITH A. PICKERING1 z 5 A Reidentification of some entries in the Ancient Star Catalog z by KEITH A. PICKERING 59 A Full speed ahead into the fog A1 The Ancient Star Catalog (ASC) appears in books 7 and 8 of Claudius Ptolemy's classic work Mathematike Syntaxis, commonly known as the Almagest. For centuries, Instructions for authors wellinformed astronomers have suspected that the catalog was plagiarized from an earlier star catalog2 by the great 2nd century BC astronomer Hipparchos of Nicaea, who worked See our requirements on the inside back cover. Contributors should send (expendable primarily on the island of Rhodes. In the 20th century, these suspicions were strongly photocopies of) papers to one of the following DIO referees — and then inquire of him by confirmed by numerical analyses put forward by Robert R. Newton and Dennis Rawlins. phone in 40 days: A2 On 15 January 2000, at the 195th meeting of the American Astronomical Society Robert Headland [polar research & exploration], Scott Polar Research Institute, University in Atlanta, Brad Schaefer (then at Yale, later Univ of Texas [later yet: Louisiana State of Cambridge, Lensfield Road, Cambridge, England CB2 1ER. -
5. Cosmic Distance Ladder Ii: Standard Candles
5. COSMIC DISTANCE LADDER II: STANDARD CANDLES EQUIPMENT Computer with internet connection GOALS In this lab, you will learn: 1. How to use RR Lyrae variable stars to measures distances to objects within the Milky Way galaxy. 2. How to use Cepheid variable stars to measure distances to nearby galaxies. 3. How to use Type Ia supernovae to measure distances to faraway galaxies. 1 BACKGROUND A. MAGNITUDES Astronomers use apparent magnitudes , which are often referred to simply as magnitudes, to measure brightness: The more negative the magnitude, the brighter the object. The more positive the magnitude, the fainter the object. In the following tutorial, you will learn how to measure, or photometer , uncalibrated magnitudes: http://skynet.unc.edu/ASTR101L/videos/photometry/ 2 In Afterglow, go to “File”, “Open Image(s)”, “Sample Images”, “Astro 101 Lab”, “Lab 5 – Standard Candles”, “CD-47” and open the image “CD-47 8676”. Measure the uncalibrated magnitude of star A: uncalibrated magnitude of star A: ____________________ Uncalibrated magnitudes are always off by a constant and this constant varies from image to image, depending on observing conditions among other things. To calibrate an uncalibrated magnitude, one must first measure this constant, which we do by photometering a reference star of known magnitude: uncalibrated magnitude of reference star: ____________________ 3 The known, true magnitude of the reference star is 12.01. Calculate the correction constant: correction constant = true magnitude of reference star – uncalibrated magnitude of reference star correction constant: ____________________ Finally, calibrate the uncalibrated magnitude of star A by adding the correction constant to it: calibrated magnitude = uncalibrated magnitude + correction constant calibrated magnitude of star A: ____________________ The true magnitude of star A is 13.74. -
The Impact of Giant Stellar Outflows on Molecular Clouds
The Impact of Giant Stellar Outflows on Molecular Clouds A thesis presented by H´ector G. Arce Nazario to The Department of Astronomy in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the subject of Astronomy Harvard University Cambridge, Massachusetts October, 2001 c 2001, by H´ector G. Arce Nazario All Rights Reserved ABSTRACT Thesis Advisor: Alyssa A. Goodman Thesis by: H´ector G. Arce Nazario We use new millimeter wavelength observations to reveal the important effects that giant (parsec-scale) outflows from young stars have on their surroundings. We find that giant outflows have the potential to disrupt their host cloud, and/or drive turbulence there. In addition, our study confirms that episodicity and a time-varying ejection axis are common characteristics of giant outflows. We carried out our study by mapping, in great detail, the surrounding molecular gas and parent cloud of two giant Herbig-Haro (HH) flows; HH 300 and HH 315. Our study shows that these giant HH flows have been able to entrain large amounts of molecular gas, as the molecular outflows they have produced have masses of 4 to 7 M |which is approximately 5 to 10% of the total quiescent gas mass in their parent clouds. These outflows have injected substantial amounts of −1 momentum and kinetic energy on their parent cloud, in the order of 10 M km s and 1044 erg, respectively. We find that both molecular outflows have energies comparable to their parent clouds' turbulent and gravitationally binding energies. In addition, these outflows have been able to redistribute large amounts of their surrounding medium-density (n ∼ 103 cm−3) gas, thereby sculpting their parent cloud and affecting its density and velocity distribution at distances as large as 1 to 1.5 pc from the outflow source. -
Constelações – Volume 8
Coleção Os Mensageiros das Estrelas: Constelações – volume 8 Constelações de Maio Organizador Paulo Henrique Colonese Autores Leonardo Pereira de Castro Rafaela Ribeiro da Silva Ilustrador Caio Lopes do Nascimento Baldi Fiocruz-COC 2021 Coleção Os Mensageiros das Estrelas: Constelações – volume 8 Constelações de Maio Organizador Paulo Henrique Colonese Autores Leonardo Pereira de Castro Rafaela Ribeiro da Silva Ilustrador Caio Lopes do Nascimento Baldi Fiocruz-COC 2021 ii Licença de Uso O conteúdo dessa obra, exceto quando indicado outra licença, está disponível sob a Licença Creative Commons, Atribuição-Não Comercial-Compartilha Igual 4.0. FUNDAÇÃO OSWALDO CRUZ Presidente Nísia Trindade Lima Diretor da Casa de Oswaldo Cruz Paulo Roberto Elian dos Santos Chefe do Museu da Vida Alessandro Machado Franco Batista TECNOLOGIAS SERVIÇO DE ITINERÂNCIA Stellarium, OBS Studio, VideoScribe, Canva CIÊNCIA MÓVEL Paulo Henrique Colonese (Coordenação) Ana Carolina de Souza Gonzalez Fernanda Marcelly de Gondra França REVISÃO CADERNO DE CONTEÚDOS Flávia Souza Lima Paulo Henrique Colonese Lais Lacerda Viana Marta Fabíola do Valle G. Mayrink APOIO ADMINISTRATIVO (Coordenação) Fábio Pimentel Paulo Henrique Colonese Rodolfo de Oliveira Zimmer MÍDIAS E DIVULGAÇÃO Julianne Gouveia CONCEPÇÃO E DESENVOLVIMENTO Melissa Raquel Faria Silva Jackson Almeida de Farias Renata Bohrer Leonardo Pereira de Castro Renata Maria B. Fontanetto (Coordenação) Luiz Gustavo Barcellos Inácio (in memoriam) Paulo Henrique Colonese (Coordenação) CAPTAÇÃO DE RECURSOS Rafaela Ribeiro da Silva Escritório de Captação da Fiocruz Willian Alves Pereira Willian Vieira de Abreu GESTÃO CULTURAL Sociedade de Promoção da Casa de Oswaldo DESIGN GRÁFICO E ILUSTRAÇÃO Cruz Caio Lopes do Nascimento Baldi Biblioteca de Educação e Divulgação Científica Iloni Seibel C756 Constelações de maio [recurso eletrônico] / Organizador: Paulo Henrique Colonese.