STELLAR EVOLUTION CODE with ROTATION Dottoranda
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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. -
Temperature, Mass and Size of Stars
Title Astro100 Lecture 13, March 25 Temperature, Mass and Size of Stars http://www.astro.umass.edu/~myun/teaching/a100/longlecture13.html Also, http://www.astro.columbia.edu/~archung/labs/spring2002/spring2002.html (Lab 1, 2, 3) Goal Goal: To learn how to measure various properties of stars 9 What properties of stars can astronomers learn from stellar spectra? Î Chemical composition, surface temperature 9 How useful are binary stars for astronomers? Î Mass 9 What is Stefan-Boltzmann Law? Î Luminosity, size, temperature 9 What is the Hertzsprung-Russell Diagram? Î Distance and Age Temp1 Stellar Spectra Spectrum: light separated and spread out by wavelength using a prism or a grating BUT! Stellar spectra are not continuous… Temp2 Stellar Spectra Photons from inside of higher temperature get absorbed by the cool stellar atmosphere, resulting in “absorption lines” At which wavelengths we see these lines depends on the chemical composition and physical state of the gas Temp3 Stellar Spectra Using the most prominent absorption line (hydrogen), Temp4 Stellar Spectra Measuring the intensities at different wavelength, Intensity Wavelength Wien’s Law: λpeak= 2900/T(K) µm The hotter the blackbody the more energy emitted per unit area at all wavelengths. The peak emission from the blackbody moves to shorter wavelengths as the T increases (Wien's law). Temp5 Stellar Spectra Re-ordering the stellar spectra with the temperature Temp-summary Stellar Spectra From stellar spectra… Surface temperature (Wien’s Law), also chemical composition in the stellar -
Stellar Evolution
Stellar Astrophysics: Stellar Evolution 1 Stellar Evolution Update date: December 14, 2010 With the understanding of the basic physical processes in stars, we now proceed to study their evolution. In particular, we will focus on discussing how such processes are related to key characteristics seen in the HRD. 1 Star Formation From the virial theorem, 2E = −Ω, we have Z M 3kT M GMr = dMr (1) µmA 0 r for the hydrostatic equilibrium of a gas sphere with a total mass M. Assuming that the density is constant, the right side of the equation is 3=5(GM 2=R). If the left side is smaller than the right side, the cloud would collapse. For the given chemical composition, ρ and T , this criterion gives the minimum mass (called Jeans mass) of the cloud to undergo a gravitational collapse: 3 1=2 5kT 3=2 M > MJ ≡ : (2) 4πρ GµmA 5 For typical temperatures and densities of large molecular clouds, MJ ∼ 10 M with −1=2 a collapse time scale of tff ≈ (Gρ) . Such mass clouds may be formed in spiral density waves and other density perturbations (e.g., caused by the expansion of a supernova remnant or superbubble). What exactly happens during the collapse depends very much on the temperature evolution of the cloud. Initially, the cooling processes (due to molecular and dust radiation) are very efficient. If the cooling time scale tcool is much shorter than tff , −1=2 the collapse is approximately isothermal. As MJ / ρ decreases, inhomogeneities with mass larger than the actual MJ will collapse by themselves with their local tff , different from the initial tff of the whole cloud. -
NGC 3105: a Young Open Cluster with Low Metallicity? J
Astronomy & Astrophysics manuscript no. 3105_aa_final c ESO 2018 May 3, 2018 NGC 3105: a young open cluster with low metallicity? J. Alonso-Santiago1, A. Marco1, I. Negueruela1, H. M. Tabernero1, N. Castro2, V. A. McBride3; 4; 5, and A. F. Rajoelimanana4; 5; 6 1 Dpto de Física, Ingeniería de Sistemas y Teoría de la Señal, Escuela Politécnica Superior, Universidad de Alicante, Carretera de San Vicente del Raspeig s/n, 03690, Spain e-mail: [email protected] 2 Department of Astronomy, University of Michigan, 1085 S. University Avenue, Ann Arbor, MI 48109-1107, USA 3 Office of Astronomy for Development, International Astronomical Union, Cape Town, South Africa 4 South African Astronomical Observatory, PO Box 9, Observatory, 7935, South Africa 5 Department of Astronomy, University of Cape Town, Private Bag X3, Rondebosch, 7701, South Africa 6 Department of Physics, University of the Free State, PO Box 339, Bloemfontein 9300, South Africa ABSTRACT Context. NGC 3105 is a young open cluster hosting blue, yellow and red supergiants. This rare combination makes it an excellent laboratory to constrain evolutionary models of high-mass stars. It is poorly studied and fundamental parameters such as its age or distance are not well defined. Aims. We intend to characterize in an accurate way the cluster as well as its evolved stars, for which we derive for the first time atmospheric parameters and chemical abundances. Methods. We performed a complete analysis combining UBVR photometry with spectroscopy. We obtained spectra with classification purposes for 14 blue stars and high-resolution spectroscopy for an in-depth analysis of the six other evolved stars. -
Calcium Triplet Synthesis
A&A manuscript no. (will be inserted by hand later) ASTRONOMY AND Your thesaurus codes are: ASTROPHYSICS () 13.2.1998 Calcium Triplet Synthesis M.L. Garc´ıa-Vargas1,2, Mercedes Moll´a3,4, and Alessandro Bressan5 1 Villafranca del Castillo Satellite Tracking Station. PO Box 50727. 28080-Madrid, Spain. 2 Present address at GTC Project, Instituto de Astrof´ısica de Canarias. V´ıa L´actea S/N. 38200 LA LAGUNA (Tenerife) 3 Dipartamento di Fisica. Universit`a di Pisa. Piazza Torricelli 2, I-56100 -Pisa, Italy 4 Present address at Departement de Physique Universit´e Laval. Chemin Sainte Foy . Quebec G1K 7P4, Canada 5 Osservatorio Astronomico di Padova. Vicolo dell’ Osservatorio 5. I-35122 -Padova, Italy. Received xxxx 1997; accepted xxxx 1998 Abstract. 1 We present theoretical equivalent widths for the sum of the two strongest lines of the Calcium Triplet, CaT index, in the near-IR (λλ 8542, 8662 A),˚ using evolutionary synthesis techniques and the most recent models and observational data for this feature in individual stars. We compute the CaT index for Single Stellar Populations (instantaneous burst, standard Salpeter-type IMF) at four different metallicities, Z=0.004, 0.008, 0.02 (solar) and 0.05, and ranging in age from very young bursts of star formation (few Myr) to old stellar populations, up to 17 Gyr, representative of galactic globular clusters, elliptical galaxies and bulges of spirals. The interpretation of the observed equivalent widths of CaT in different stellar systems is discussed. Composite-population models are also computed as a tool to interpret the CaT detections in star-forming regions, in order to disentangle between the component due to Red Supergiant stars, RSG, and the underlying, older, population. -