Glossary/Print.Php?Id=322668&Mode=Lett

Total Page:16

File Type:pdf, Size:1020Kb

Glossary/Print.Php?Id=322668&Mode=Lett http://learn.open.ac.uk/mod/glossary/print.php?id=322668&mode=lett... Tuesday, 3 August 2010, 17:04 Site: OU online Course: Astrophysics (S382-10B) Glossary: Glossary 1 1 micron minimum: A local minimum in the continuum spectrum of most AGN occurring around a wavelength of 1 micron (1 µm). It is thought to represent the minimum between a hot thermal spectrum (the big blue bump) possibly due to emission from an accretion disc, and a cool thermal spectrum due to emission in the infrared by warm dust grains. 2 2dF: The 2 degree field multi-object spectrometer on the Anglo Australian Telescope. Used to conduct the 2dF galaxy redshift survey and the 2dF quasar survey. 2MASS: The 2 Micron All Sky Survey. A survey of the complete sky using two telescopes (one at Mount Hopkins, Arizona and one at Cerro-Tololo, Chile) in three infrared wavebands: J-band (1.25 µm), H-band (1.65 µm) and K-band (2.17 µm). 3 3C273: One of the closest quasars to us (redshift = 0.158), the optically brightest (magnitude = 12.9) and the first quasar to be identified, in the 3C radio source catalogue. 4 4000 angstrom break: A break, or absorption feature, at a wavelength of 4000Å in the spectra of galaxies caused by Balmer continuum absorption in the atmospheres of stars. A aberration of light: The phenomenon whereby the observed direction of a star changes with time, due to the combined effect of the motion of the observer and the finite speed of light. If the relative speed of the observer and star is small compared to the speed of light, the aberration is small: tan α = (v/c)sin θ, where α is the aberration angle, v is the speed of motion, c is the speed of light and θ is the angle between the direction of motion and the direction of the star. The aberration due to the Earth’s motion around the Sun is no more than 20.5 arc seconds. If the relative speeds are a significant fraction of the speed of light, the effects of special relativity become significant and the Lorentz transformations must be used to calculate the aberration angle. ablation: The process whereby material is lost from a body as a result of gas or fluid flow past it. The gas carries away (ablates) material from the body’s surface. absolute magnitude: A numerical quantity used to describe the luminosity of a body. The relationship between absolute magnitude and luminosity is given by: M = -2.5 log10 L + K where K is a constant that depends on the units of L and the waveband being considered. The absolute magnitude of an astronomical body is equal to the apparent magnitude the body would have if it were located at a distance of 10 parsecs from the observer, ignoring any effects due to obscuration. absolute temperature: Any temperature measured on the thermodynamic temperature scale. absolute temperature scale: See thermodynamic temperature scale. absolute visual magnitude: An absolute magnitude, measured in the visual (V) band (at wavelengths around 550 nm). absorption (and emission) of radiation: General processes whereby energy carried by electromagnetic radiation may be added to, or taken from, the total energy of the system responsible for the emission or absorption. A particular case is that in which an electron makes a radiative transition between two energy levels in an atom. When an electron makes a transition from a lower energy level E1 to a higher energy level E2, the atom increases its total energy by an amount E2 - E1. In the case of a radiative transition, the atom obtains this energy by absorbing a single photon of energy E2 - E1. Similarly, an atom can emit a photon of energy E2 - E1 in a radiative transition when one of its electrons makes a transition from a higher energy level E2 to a lower energy level E1. 1 of 142 Copyright © 2010 The Open University 03/08/20101 17:07 http://learn.open.ac.uk/mod/glossary/print.php?id=322668&mode=lett... absorption distance: The quantity X in the expression If absorbers have a constant comoving space density and constant proper sizes and cross sections, then the number of absorbers per unit absorption distance is constant. absorption edge: A jump in absorption cross-section at a particular wavelength or energy corresponding to an ionisation state of the absorbing atom or ion. absorption line: See absorption line spectrum. absorption line spectrum: A spectrum of the kind observed when continuum radiation (e.g. from a black body) passes through matter. Radiation is absorbed at specific energies (wavelengths) corresponding to atomic or molecular transitions in the absorbing material, giving rise to absorption lines in the spectrum (see, for example, hydrogen spectrum). The absorption spectrum gives information on the atomic or molecular species present and their physical state. accelerating model: A model of the universe in which the rate of expansion increases. The acceleration is a result of the changing densities of matter, radiation and dark energy with time. acceleration: The (instantaneous) rate of change of velocity of a body. For a particle moving in one-dimension along the x-axis, the acceleration ax at any time is the instantaneous rate of change of the particle’s velocity vx, and is given by the gradient of the particle’s velocity–time graph at the relevant time. This gradient is equal to the derivative of the velocity with respect to time at the relevant time, so the acceleration at time t may be written Acceleration is a vector quantity, characterized by a direction as well as a magnitude. In one dimension the sign of ax suffices to indicate the direction, but in two or three dimensions some other method must be used to indicate direction. This is often achieved by expressing the acceleration vector in terms of its (Cartesian) components, as in a = (ax, ay, az), where and v(t) is the velocity vector. acceleration due to gravity: The acceleration towards the centre of a massive body (such as a star or planet) of a freely falling object. The magnitude of the acceleration for a spherically symmetrical body is GM/r2, where M is the mass of the body inside the radius r, r is the distance from the centre of mass and G is the universal gravitational constant. The acceleration is independent of the mass of the falling object, and so is the same for all bodies in the same gravitational field. At the surface of the Earth the magnitude of the acceleration due to the Earth’s gravity is about 9.81 m s-2. This quantity varies slightly from place to place, but is generally represented by the symbol g. accretion: The process whereby the mass of an astronomical body grows as a result of the accumulation of matter. Accretion is most important in systems where matter is falling in under the influence of gravity; it allows a massive body to gain more mass from other matter in its surroundings. If the infalling matter has significant angular momentum, an accretion disc is formed. The luminosity of various types of astronomical object, including X-ray binaries and active galactic nuclei, is ultimately the result of accretion. accretion column: A form of accretion flow where the width in any direction perpendicular to the direction of the flow is small compared to the geometrical extent along the flow direction. The magnetically controlled accretion in polars is thought to occur via an accretion column. accretion curtain: A form of accretion flow between the inner edge of a magnetically disrupted accretion disc and the surface of the accretor. The magnetically controlled accretion in intermediate polars is thought to occur via accretion curtains. accretion disc: A flow of matter that is largely confined to a plane and that is spiralling in towards a central object. The azimuthal component of the flow velocity is close to the Keplerian value, while the radial component is much smaller. See also mass transfer. accretion disc luminosity: 2 of 142 Copyright © 2010 The Open University 03/08/20102 17:07 http://learn.open.ac.uk/mod/glossary/print.php?id=322668&mode=lett... The energy an accretion disc radiates per unit time. For a steady-state, geometrically thin, optically thick, infinite disc with a non-rotating central accretor with mass M and radius R* and accretion rate , the accretion disc luminosity is (G is the gravitational constant). This is just half the accretion luminosity. accretion disc spectrum: The continuum spectrum of a geometrically thin, optically thick, Keplerian, steady state accretion disc is a ‘stretched-out’ black body spectrum, with a characteristic flat region 1/3 where Fν ∝ ν accretion disc structure: See accretion disc. accretion efficiency: The accretion luminosity, expressed in units of the rate of accreted mass energy. If Lacc denotes the accretion luminosity, the mass accretion rate, and c the speed of light, then the accretion efficiency is . accretion luminosity: The gravitational energy liberated by accretion per unit time. If an object with mass M and radius R* accretes matter at a rate the accretion luminosity is (G is the gravitational constant). accretion powered compact binaries: See X-ray binary, cataclysmic variable. accretion powered compact binary: See X-ray binary; cataclysmic variable. accretion powered pulsar: A pulsar whose emission is powered by accretion from a companion star. See X-ray pulsar. accretion rate: The mass accumulated per unit time through accretion. Usually denoted by and –1 –1 –1 measured in kg s or g s or M0 yr (sometimes also called mass accretion rate).
Recommended publications
  • Arxiv:2007.13451V2 [Gr-Qc] 24 Nov 2020 on GR and Its Modifications [31–33], but Also Delivers Model Particles As Well As Dark Matter Candidates [56– Drawbacks
    Early evolutionary tracks of low-mass stellar objects in modified gravity Aneta Wojnar1, ∗ 1Laboratory of Theoretical Physics, Institute of Physics, University of Tartu, W. Ostwaldi 1, 50411 Tartu, Estonia Using a simple model of low-mass stellar objects we have shown modified gravity impact on their early evolution, such as Hayashi tracks, radiative core development, effective temperature, masses, and luminosities. We have also suggested that the upper mass' limit of fully convective stars on the Main Sequence might be different than commonly adopted. I. INTRODUCTION is, in the so-called mass gap [38]), which merged with a black hole of 23M , provided even more questions for Working on modified gravity does not make one to for- theoretical physics of compact objects. get the elegance and success of Einstein's theory of grav- However, it turns out that there is a class of stellar ity, being already confirmed by many observations [1]; objects, with the internal structure much better under- even more, General Relativity (GR) still delights when stood than that of neutron stars, which might be used to one of its mysterious predictions, such as the existence of constrain theories of gravity. It is a family of low-mass black holes, is directly affirmed by the finding of gravi- stars (LMS) [39{41] which includes such ordinary objects tational waves as a result of black holes' binary mergers as M dwarfs (also called red dwarfs), which are cool Main [2] as well as soon after the imaging of the shadow of the Sequence stars with masses in the range [0:09 − 0:6]M , supermassive black hole of M87 [3] (see [4] for a review).
    [Show full text]
  • Revisiting the Pre-Main-Sequence Evolution of Stars I. Importance of Accretion Efficiency and Deuterium Abundance ?
    Astronomy & Astrophysics manuscript no. Kunitomo_etal c ESO 2018 March 22, 2018 Revisiting the pre-main-sequence evolution of stars I. Importance of accretion efficiency and deuterium abundance ? Masanobu Kunitomo1, Tristan Guillot2, Taku Takeuchi,3,?? and Shigeru Ida4 1 Department of Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Aichi 464-8602, Japan e-mail: [email protected] 2 Université de Nice-Sophia Antipolis, Observatoire de la Côte d’Azur, CNRS UMR 7293, 06304 Nice CEDEX 04, France 3 Department of Earth and Planetary Sciences, Tokyo Institute of Technology, 2-12-1 Ookayama, Meguro-ku, Tokyo 152-8551, Japan 4 Earth-Life Science Institute, Tokyo Institute of Technology, 2-12-1 Ookayama, Meguro-ku, Tokyo 152-8551, Japan Received 5 February 2016 / Accepted 6 December 2016 ABSTRACT Context. Protostars grow from the first formation of a small seed and subsequent accretion of material. Recent theoretical work has shown that the pre-main-sequence (PMS) evolution of stars is much more complex than previously envisioned. Instead of the traditional steady, one-dimensional solution, accretion may be episodic and not necessarily symmetrical, thereby affecting the energy deposited inside the star and its interior structure. Aims. Given this new framework, we want to understand what controls the evolution of accreting stars. Methods. We use the MESA stellar evolution code with various sets of conditions. In particular, we account for the (unknown) efficiency of accretion in burying gravitational energy into the protostar through a parameter, ξ, and we vary the amount of deuterium present. Results. We confirm the findings of previous works that, in terms of evolutionary tracks on the Hertzsprung-Russell (H-R) diagram, the evolution changes significantly with the amount of energy that is lost during accretion.
    [Show full text]
  • HI Balmer Jump Temperatures for Extragalactic HII Regions in the CHAOS Galaxies
    HI Balmer Jump Temperatures for Extragalactic HII Regions in the CHAOS Galaxies A Senior Thesis Presented in Partial Fulfillment of the Requirements for Graduation with Research Distinction in Astronomy in the Undergraduate Colleges of The Ohio State University By Ness Mayker The Ohio State University April 2019 Project Advisors: Danielle A. Berg, Richard W. Pogge Table of Contents Chapter 1: Introduction ............................... 3 1.1 Measuring Nebular Abundances . 8 1.2 The Balmer Continuum . 13 Chapter 2: Balmer Jump Temperature in the CHAOS galaxies .... 16 2.1 Data . 16 2.1.1 The CHAOS Survey . 16 2.1.2 CHAOS Balmer Jump Sample . 17 2.2 Balmer Jump Temperature Determinations . 20 2.2.1 Balmer Continuum Significance . 20 2.2.2 Balmer Continuum Measurements . 21 + 2.2.3 Te(H ) Calculations . 23 2.2.4 Photoionization Models . 24 2.3 Results . 26 2.3.1 Te Te Relationships . 26 − 2.3.2 Discussion . 28 Chapter 3: Conclusions and Future Work ................... 32 1 Abstract By understanding the observed proportions of the elements found across galaxies astronomers can learn about the evolution of life and the universe. Historically, there have been consistent discrepancies found between the two main methods used to measure gas-phase elemental abundances: collisionally excited lines and optical recombination lines in H II regions (ionized nebulae around young star-forming regions). The origin of the discrepancy is thought to hinge primarily on the strong temperature dependence of the collisionally excited emission lines of metal ions, principally Oxygen, Nitrogen, and Sulfur. This problem is exacerbated by the difficulty of measuring ionic temperatures from these species.
    [Show full text]
  • Single Star Implementation Notes
    Mon. Not. R. Astron. Soc. 000, 000{000 (0000) Printed 8 November 2017 (MN LATEX style file v2.2) Single Star Implementation Notes PFH 8 November 2017 1 METHODS 1=2 − 1 times the cloud diameter Lcloud) are driven as an Ornstein-Uhlenbeck process in Fourier space, with the com- Our simulations use GIZMO (?),1, and include full self- pressive part of the modes projected out via Helmholtz de- gravity, adaptive resolution, ideal and non-ideal magneto- composition so that we can specify the ratio of compress- hydrodynamics (MHD), detailed cooling and heating ible and incompressible/solenoidal modes. Unless otherwise physics, protostar formation, accretion, and feedback in the specified we adopt pure solenoidal driving, appropriate for form of protostellar jets and radiative heating, and main- e.g. galactic shear (so that we do not artificially \force" com- sequence stellar feedback in the form of photo-ionization pression/collapse), but we vary this. The specific implemen- and photo-electric heating, radiation pressure, stellar winds, tation here has been verified in ????. and supernovae. A subset of our runs include explicit treat- The driving specifies the large-scale steady-state (one- ment of the dust particle and cosmic ray dynamics as well dimensional) turbulent velocity σ ≡ hv2 i1=2 and as radiation-hydrodynamics; otherwise these are included in 1D turb; 1D Mach number M ≡ h(v =c )2i1=2, where v is simplified form. turb; 1D s turb; 1D an (arbitrary) projection (in detail we average over all 1.1 Gravity random projections). Unless otherwise specified, we initial- ize our clouds on the linewidth-size relation from ?, with All our simulations include full self-gravity for gas, stars, −1 1=2 σ1D ≈ 0:7 km s (Lcloud=pc) and dust.
    [Show full text]
  • 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
    [Show full text]
  • The Physics of the Accretion Process in the Formation and Evolution of Young Stellar Objects
    The physics of the accretion process in the formation and evolution of Young Stellar Objects Carlo Felice Manara München 2014 The physics of the accretion process in the formation and evolution of Young Stellar Objects Carlo Felice Manara Dissertation an der Fakultät für Physik der Ludwig--Maximilians--Universität München vorgelegt von Carlo Felice Manara aus Mailand, Italien München, den 22. Maj 2014 Erstgutachter: Prof. Dr. Barbara Ercolano Zweitgutachter: Prof. Dr. Andreas Burkert Tag der mündlichen Prüfung: 8. Juli 2014 To my two girls This work has been carried out at the European Southern Observatory (ESO) under the su- pervision of Leonardo Testi and within the ESO/International Max Planck Research School (IMPRS) student fellowship programme. The members of the Thesis Committee were: Barbara Ercolano, Leonardo Testi, Thomas Preibisch, and Antonella Natta. vi Contents Abstract xvii Zusammenfassung xvii List of Acronyms xxi 1 Introduction 1 1.1 Setting the scene: the evolutionary path from molecular cloud cores to stars and planets ................................... 1 1.2 Star-disk interaction: accretion ......................... 5 1.2.1 Magnetospheric accretion ....................... 5 1.3 Accretion as a tracer of protoplanetary disk evolution ............ 7 1.3.1 Evolution of accretion rates with time in a viscous disk ....... 7 1.3.2 Evolution of accretion rates with time due to photoevaporation ... 13 1.3.3 The dependence of accretion rates with the mass of the central star . 15 1.4 The role of this Thesis .............................. 20 1.4.1 The state of the art at the beginning of this Thesis ........... 20 1.4.2 Open issues at the beginning of this Thesis .............
    [Show full text]
  • An Analysis of the Shapes of Interstellar Extinction Curves. VII
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Ghent University Academic Bibliography The Astrophysical Journal, 886:108 (24pp), 2019 December 1 https://doi.org/10.3847/1538-4357/ab4c3a © 2019. The American Astronomical Society. All rights reserved. An Analysis of the Shapes of Interstellar Extinction Curves. VII. Milky Way Spectrophotometric Optical-through-ultraviolet Extinction and Its R-dependence* E. L. Fitzpatrick1 , Derck Massa2 , Karl D. Gordon3,4 , Ralph Bohlin3 , and Geoffrey C. Clayton5 1 Department of Astrophysics & Planetary Science, Villanova University, 800 Lancaster Avenue, Villanova, PA 19085, USA 2 Space Science Institute 4750 Walnut Street, Suite 205 Boulder, CO 80301, USA; [email protected] 3 Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218, USA 4 Sterrenkundig Observatorium, Universiteit Gent, Gent, Belgium 5 Department of Physics & Astronomy, Louisiana State University, Baton Rouge, LA 70803, USA Received 2019 September 20; revised 2019 October 7; accepted 2019 October 8; published 2019 November 26 Abstract We produce a set of 72 NIR-through-UV extinction curves by combining new Hubble Space Telescope/STIS optical spectrophotometry with existing International Ultraviolet Explorer spectrophotometry (yielding gapless coverage from 1150 to 10000 Å) and NIR photometry. These curves are used to determine a new, internally consistent NIR-through-UV Milky Way mean curve and to characterize how the shapes of the extinction curves depend on R(V ). We emphasize that while this dependence captures much of the curve variability, considerable variation remains that is independent of R(V ). We use the optical spectrophotometry to verify the presence of structure at intermediate wavelength scales in the curves.
    [Show full text]
  • 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.
    [Show full text]
  • Ast 777: Star and Planet Formation Pre-Main Sequence Stars and the IMF
    Ast 777: Star and Planet Formation Pre-main sequence stars and the IMF https://universe-review.ca/F08-star05.htm The main phases of star formation https://www.americanscientist.org/sites/americanscientist.org/files/2005223144527_306.pdf The star has formed* but is not yet on the MS * it has attained its final mass (or ~99% of it) https://www.americanscientist.org/sites/americanscientist.org/files/2005223144527_306.pdf The star is optically visible and is a Class II or III star (or TTS or HAeBe) https://www.americanscientist.org/sites/americanscientist.org/files/2005223144527_306.pdf PMS evolution is described by the equations of stellar evolution But there are differences from MS evolution: ‣ initial conditions are very different from the MS (and have significant uncertainties) ‣ energy is produced by gravitational collapse and deuterium burning (This was mostly figured out 30-50 years ago so the references are old, but important for putting current work in context) But see later… How big is a star when the core stops collapsing? Upper limit can be determined by assuming that all the gravitational energy of the core is used to dissociate and ionized the H2+He gas (i.e., no radiative losses during collapse) Each H2 requires 4.48eV to dissociate —> this produces a short-lived intermediate step along the way to a protostar, called the first hydrostatic core (hinted at, though not definitively confirmed, through FIR/mm observations) How big is a star when the core stops collapsing? Upper limit can be determined by assuming that all the gravitational
    [Show full text]
  • The Influence of Radiative Core Growth on Coronal X-Ray Emission from Pre
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE MNRAS Advance Access published February 2, 2016 provided by St Andrews Research Repository MNRAS 000, 1–22 (2015) Preprint 30 January 2016 Compiled using MNRAS LATEX style file v3.0 The influence of radiative core growth on coronal X-ray emission from pre-main sequence stars Scott G. Gregory,1? Fred C. Adams2;3 and Claire L. Davies4;1 1SUPA, School of Physics & Astronomy, University of St Andrews, St Andrews, KY16 9SS, U.K. 2Physics Department, University of Michigan, Ann Arbor, MI 48109, U.S.A. 3Astronomy Department, University of Michigan, Ann Arbor, MI 48109, U.S.A. 4School of Physics, University of Exeter, Exeter, EX4 4QL, U.K. Downloaded from Accepted XXX. Received YYY; in original form ZZZ ABSTRACT Pre-main sequence (PMS) stars of mass & 0:35 M transition from hosting fully convective interiors to configurations with a radiative core and outer convective envelope during their http://mnras.oxfordjournals.org/ gravitational contraction. This stellar structure change influences the external magnetic field topology and, as we demonstrate herein, affects the coronal X-ray emission as a stellar analog of the solar tachocline develops. We have combined archival X-ray, spectroscopic, and photo- metric data for ∼1000 PMS stars from five of the best studied star forming regions; the ONC, NGC 2264, IC 348, NGC 2362, and NGC 6530. Using a modern, PMS calibrated, spectral type-to-effective temperature and intrinsic colour scale, we deredden the photometry using colours appropriate for each spectral type, and determine the stellar mass, age, and internal structure consistently for the entire sample.
    [Show full text]
  • Understanding the Luminosity and Surface Temperature of Stars
    Understanding the Luminosity and Surface Temperature of Stars 1. The Hertsprung-Russell diagram Astronomers like to plot the evolution of stars on what is known as the Hertsprung- Russell diagram. Modern versions of this diagram plot the luminosity of the star against its surface temperature, so to understand how a star moves on this diagram as it ages, we need to understand the physics that sets the luminosity and surface temperature of stars. Surprisingly, these can be understood at an approximate level using only basic physics, over most of the evolution of both low-mass and high-mass stars. 2. The role of heat loss Stellar evolution is fundamentally the story of what happens to a star by virtue of it losing an enormous amount of heat. By the virial theorem, the total kinetic energy in a star equals half its total gravitational potential energy (in absolute value), as long as the gas in the star remains nonrelativistic. This implies that when a gravitationally bound object loses heat by shining starlight, it always contracts to a state of higher internal kinetic energy. For a nonrelativistic gas, the pressure P is related to the kinetic energy density KE/V by 2 KE P = , (1) 3 V we can apply the nonrelativistic virial theorem KE 1 GMm = i (2) N 2 R where mi is the average ion mass (about the mass of a proton, usually) to assert that the characteristic pressure over the interior (i.e., the core pressure Pc) approximates GMρ 2 P ∼ ∝ , (3) c R R4 where ρ ∝ M/R3 is the mass density.
    [Show full text]
  • Rest-Frame Ultraviolet-To-Optical Spectral Characteristics of Extremely Metal-Poor and Metal-Free Galaxies Akio K
    Mon. Not. R. Astron. Soc. 415, 2920–2931 (2011) doi:10.1111/j.1365-2966.2011.18906.x Rest-frame ultraviolet-to-optical spectral characteristics of extremely metal-poor and metal-free galaxies Akio K. Inoue College of General Education, Osaka Sangyo University, 3-1-1 Nakagaito, Daito, Osaka 574-8530, Japan Accepted 2011 April 12. Received 2011 March 31; in original form 2011 January 28 Downloaded from https://academic.oup.com/mnras/article/415/3/2920/1054046 by guest on 29 September 2021 ABSTRACT Finding the first generation of galaxies in the early Universe is the greatest step forward towards understanding galaxy formation and evolution. For a strategic survey of such galaxies and the interpretation of the obtained data, this paper presents an ultraviolet-to-optical spectral model of galaxies with a great care of the nebular emission. In particular, we present a machine- readable table of intensities of 119 nebular emission lines from Lyα to the rest-frame 1 µmas a function of metallicity from zero to the solar one. Based on the spectral model, we present criteria of equivalent widths of Lyα,HeII λ1640, Hα,Hβ and [O III] λ5007 to select extremely metal-poor and metal-free galaxies although these criteria have uncertainty caused by the Lyman continuum escape fraction and the star formation duration. We also present criteria of broad-band colours which will be useful to select candidates for spectroscopic follow-up from drop-out galaxies. We propose the line intensity ratio of [O III] λ5007 to Hβ<0.1 as the most robust criterion for <1/1000 of the solar metallicity.
    [Show full text]