Stellar Evolution
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Star Formation and Mass Assembly in High Redshift Galaxies
A&A 504, 751–767 (2009) Astronomy DOI: 10.1051/0004-6361/200811434 & c ESO 2009 Astrophysics Star formation and mass assembly in high redshift galaxies P. Santini1,2,A.Fontana1, A. Grazian1,S.Salimbeni1,3, F. Fiore1, F. Fontanot4, K. Boutsia1, M. Castellano1,2, S. Cristiani5, C. De Santis6,7, S. Gallozzi1, E. Giallongo1, N. Menci1, M. Nonino5, D. Paris1, L. Pentericci1, and E. Vanzella5 1 INAF – Osservatorio Astronomico di Roma, via Frascati 33, 00040 Monteporzio (RM), Italy e-mail: [email protected] 2 Dipartimento di Fisica, Università di Roma “La Sapienza”, P.le A. Moro 2, 00185 Roma, Italy 3 Department of Astronomy, University of Massachusetts, 710 North Pleasant Street, Amherst, MA 01003, USA 4 MPIA Max-Planck-Institute für Astronomie, Koenigstuhl 17, 69117 Heidelberg, Germany 5 INAF – Osservatorio Astronomico di Trieste, via G.B. Tiepolo 11, 34131 Trieste, Italy 6 Dip. di Fisica, Università Tor Vergata, via della Ricerca Scientifica 1, 00133 Roma, Italy 7 INFN – Roma Tor Vergata, via della Ricerca Scientifica 1, 00133 Roma, Italy Received 27 November 2008 / Accepted 24 April 2009 ABSTRACT Aims. The goal of this work is to infer the star formation properties and the mass assembly process of high redshift (0.3 ≤ z < 2.5) galaxies from their IR emission using the 24 μm band of MIPS-Spitzer. Methods. We used an updated version of the GOODS-MUSIC catalog, which has multiwavelength coverage from 0.3 to 24 μmand either spectroscopic or accurate photometric redshifts. We describe how the catalog has been extended by the addition of mid-IR fluxes derived from the MIPS 24 μm image. -
Luminous Blue Variables
Review Luminous Blue Variables Kerstin Weis 1* and Dominik J. Bomans 1,2,3 1 Astronomical Institute, Faculty for Physics and Astronomy, Ruhr University Bochum, 44801 Bochum, Germany 2 Department Plasmas with Complex Interactions, Ruhr University Bochum, 44801 Bochum, Germany 3 Ruhr Astroparticle and Plasma Physics (RAPP) Center, 44801 Bochum, Germany Received: 29 October 2019; Accepted: 18 February 2020; Published: 29 February 2020 Abstract: Luminous Blue Variables are massive evolved stars, here we introduce this outstanding class of objects. Described are the specific characteristics, the evolutionary state and what they are connected to other phases and types of massive stars. Our current knowledge of LBVs is limited by the fact that in comparison to other stellar classes and phases only a few “true” LBVs are known. This results from the lack of a unique, fast and always reliable identification scheme for LBVs. It literally takes time to get a true classification of a LBV. In addition the short duration of the LBV phase makes it even harder to catch and identify a star as LBV. We summarize here what is known so far, give an overview of the LBV population and the list of LBV host galaxies. LBV are clearly an important and still not fully understood phase in the live of (very) massive stars, especially due to the large and time variable mass loss during the LBV phase. We like to emphasize again the problem how to clearly identify LBV and that there are more than just one type of LBVs: The giant eruption LBVs or h Car analogs and the S Dor cycle LBVs. -
SHELL BURNING STARS: Red Giants and Red Supergiants
SHELL BURNING STARS: Red Giants and Red Supergiants There is a large variety of stellar models which have a distinct core – envelope structure. While any main sequence star, or any white dwarf, may be well approximated with a single polytropic model, the stars with the core – envelope structure may be approximated with a composite polytrope: one for the core, another for the envelope, with a very large difference in the “K” constants between the two. This is a consequence of a very large difference in the specific entropies between the core and the envelope. The original reason for the difference is due to a jump in chemical composition. For example, the core may have no hydrogen, and mostly helium, while the envelope may be hydrogen rich. As a result, there is a nuclear burning shell at the bottom of the envelope; hydrogen burning shell in our example. The heat generated in the shell is diffusing out with radiation, and keeps the entropy very high throughout the envelope. The core – envelope structure is most pronounced when the core is degenerate, and its specific entropy near zero. It is supported against its own gravity with the non-thermal pressure of degenerate electron gas, while all stellar luminosity, and all entropy for the envelope, are provided by the shell source. A common property of stars with well developed core – envelope structure is not only a very large jump in specific entropy but also a very large difference in pressure between the center, Pc, the shell, Psh, and the photosphere, Pph. Of course, the two characteristics are closely related to each other. -
1 Firm and Less Firm Outcomes of Stellar Evolution Theory
i i Laura Greggio and Alvio Renzini: Stellar Populations — Chap. renzini9181c01 — 2011/7/12 — page 1 — le-tex i i 1 1 Firm and Less Firm Outcomes of Stellar Evolution Theory Stellar evolution theory is a mature science which provides the backbone to the theory of stellar populations and the construction of their synthetic luminosities, colors and spectra. In turn, synthetic stellar populations offer the virtually unique possibility to estimate the ages of stellar systems from star clusters to whole galax- ies, their star formation rates and star formation histories, and their mass in stars. This chapter is no substitute to a whole textbook on stellar evolution, of which there are many. It rather offers an introduction to stellar evolution, meant to familiarize the reader with the pertinent nomenclature and a few key concepts. Particular at- tention is devoted to highlight the strengths and weaknesses of current methods, assumptions and results of stellar evolution theory, in particular concerning their impact on synthetic stellar populations. Further readings on the treated issues are listed at the end of this chapter. 1.1 A Brief Journey through Stellar Evolution 1.1.1 A9Mˇ Star Figure 1.1 shows the calculated evolutionary path on the Hertzsprung–Russell di- agram (HRD) of a 9 Mˇ star of solar composition. Letters mark critical points in thecourseofevolutionandTable1.1givesthe corresponding times to reach them. Specifically, the various points mark the following events: A: Beginning of steady hydrogen burning, zero age main sequence (ZAMS). C-C0: Exhaustion of hydrogen in the core, and ignition of hydrogen burning in a shell surrounding the hydrogen-exhausted core. -
The Endpoints of Stellar Evolution Answer Depends on the Star’S Mass Star Exhausts Its Nuclear Fuel - Can No Longer Provide Pressure to Support Itself
The endpoints of stellar evolution Answer depends on the star’s mass Star exhausts its nuclear fuel - can no longer provide pressure to support itself. Gravity takes over, it collapses Low mass stars (< 8 Msun or so): End up with ‘white dwarf’ supported by degeneracy pressure. Wide range of structure and composition!!! Answer depends on the star’s mass Star exhausts its nuclear fuel - can no longer provide pressure to support itself. Gravity takes over, it collapses Higher mass stars (8-25 Msun or so): get a ‘neutron star’ supported by neutron degeneracy pressure. Wide variety of observed properties Answer depends on the star’s mass Star exhausts its nuclear fuel - can no longer provide pressure to support itself. Gravity takes over, it collapses Above about 25 Msun: we are left with a ‘black hole’ Black holes are astounding objects because of their simplicity (consider all the complicated physics to set all the macroscopic properties of a star that we have been through) - not unlike macroscopic elementary particles!! According to general relativity, the black hole properties are set by two numbers: mass and spin change of photon energies towards the gravitating mass the opposite when emitted Pound-Rebka experiment used atomic transition of Fe Important physical content for BH studies: general relativity has no intrisic scale instead, all important lengthscales and timescales are set by - and become proportional to the mass. Trick… Examine the energy… Why do we believe that black holes are inevitably created by gravitational collapse? Rather astounding that we go from such complicated initial conditions to such “clean”, simple objects! . -
Stars IV Stellar Evolution Attendance Quiz
Stars IV Stellar Evolution Attendance Quiz Are you here today? Here! (a) yes (b) no (c) my views are evolving on the subject Today’s Topics Stellar Evolution • An alien visits Earth for a day • A star’s mass controls its fate • Low-mass stellar evolution (M < 2 M) • Intermediate and high-mass stellar evolution (2 M < M < 8 M; M > 8 M) • Novae, Type I Supernovae, Type II Supernovae An Alien Visits for a Day • Suppose an alien visited the Earth for a day • What would it make of humans? • It might think that there were 4 separate species • A small creature that makes a lot of noise and leaks liquids • A somewhat larger, very energetic creature • A large, slow-witted creature • A smaller, wrinkled creature • Or, it might decide that there is one species and that these different creatures form an evolutionary sequence (baby, child, adult, old person) Stellar Evolution • Astronomers study stars in much the same way • Stars come in many varieties, and change over times much longer than a human lifetime (with some spectacular exceptions!) • How do we know they evolve? • We study stellar properties, and use our knowledge of physics to construct models and draw conclusions about stars that lead to an evolutionary sequence • As with stellar structure, the mass of a star determines its evolution and eventual fate A Star’s Mass Determines its Fate • How does mass control a star’s evolution and fate? • A main sequence star with higher mass has • Higher central pressure • Higher fusion rate • Higher luminosity • Shorter main sequence lifetime • Larger -
Pop III Binary Population Synthesis
Remnants of first stars for gravitational wave sources Tomoya Kinugawa Institute for Cosmic Ray Research The University of Tokyo collaborators: T. Nakamura, K. Inayoshi, K. Hotokezaka, D. Nakauchi A. Miyamoto, N. Kanda, A. Tanikawa, T. Yoshida The beginning of Gravitational wave astronomy • Gravitational wave detectors KAGRA Advanced LIGO Advanced VIRGO ©VIRGO ©KAGRA ©LIGO Masses of GW events • GW events show that there are many massive BHs (≳30 Msun). • 7/10 BBHs are massive BBHs • On the other hand, the typical mass of BHs in X-ray binaries is ~10 Msun. The LIGO scientific collaboration 2018 Origin of massive BBHs 7/10 GW BBHs are massive BBHs In order to explain the origin of such massive BBHs Many theories exist such as • 1)Pop II BBH • 2)Pop III BBH No metal field binaries • 3)Primordial Binary BH • 4)N body origin from Globular Cluster • ……………………. Pop III binary population synthesis We simulate 106 Pop III-binary evolutions and estimate how many binaries become compact binary which merges within Hubble time. ×84 models (Kinugawa et al.2014, 2016) Initial stellar parameters are decided by Monte Carlo method with initial distribution functions • Initial parameter (M1,M2,a,e) distribution in our standard model M1 : Flat (10 M<M<100 M) q=M2/M1 : P(q)=const. (0<q<1) The same distribution functions 6 adopted for Pop I population a : P(a)∝1/a (amin<a<10 R) synthesis e : P(e)∝e (0<e<1) • de Souza SFR Total mass distribution of BBH which merge within the Hubble time Typical total mass M~60 M Z=0 (Pop III) (30 M +30 M) TK et al. -
Chapter 16 the Sun and Stars
Chapter 16 The Sun and Stars Stargazing is an awe-inspiring way to enjoy the night sky, but humans can learn only so much about stars from our position on Earth. The Hubble Space Telescope is a school-bus-size telescope that orbits Earth every 97 minutes at an altitude of 353 miles and a speed of about 17,500 miles per hour. The Hubble Space Telescope (HST) transmits images and data from space to computers on Earth. In fact, HST sends enough data back to Earth each week to fill 3,600 feet of books on a shelf. Scientists store the data on special disks. In January 2006, HST captured images of the Orion Nebula, a huge area where stars are being formed. HST’s detailed images revealed over 3,000 stars that were never seen before. Information from the Hubble will help scientists understand more about how stars form. In this chapter, you will learn all about the star of our solar system, the sun, and about the characteristics of other stars. 1. Why do stars shine? 2. What kinds of stars are there? 3. How are stars formed, and do any other stars have planets? 16.1 The Sun and the Stars What are stars? Where did they come from? How long do they last? During most of the star - an enormous hot ball of gas day, we see only one star, the sun, which is 150 million kilometers away. On a clear held together by gravity which night, about 6,000 stars can be seen without a telescope. -
The Great Supernova of 1987
The great supernova of 1987 SN 1987 A. Despite their apparently very different objectives, astrophy sics - the study of the largest structures in the Universe - and particle physics - the study of the smallest - have always had common ground. On 23 February 1987 a super nova explosion provided addi tional impetus to reinforce these links. In this article, David Schramm of the Univer sity of Chicago and the NASA/Fermilab Astrophysics Center, explains why. One of the most spectacular events in modern astrophysics occurred on 23 February 1987, when light and neutrinos from a supernova ex plosion in the Large Magellanic Cloud (LMC) first reached Earth. The LMC (a satellite of our Milky Way Galaxy) is 170,000 light years away, making the event, code- named SN 1987A, the closest vi sual supernova since Kepler ob served one almost 400 years ago. Most of our knowledge of super- novae has come either from obser vations of outbursts in distant gal axies, too far away to obtain neu trinos, or from studies of old rem nants in our Galaxy, thus missing the fireworks. Having a supernova blast off re also proved that our ideas about novae that were missed in previous latively nearby while neutrino and element formation in exploding supernova rate estimates. Another electromagnetic radiation detectors stars were basically correct. In par exciting ingredient was the recent were in action has been fantastic. ticular, the gamma rays from ra report of a 0.5 ms pulsar remnant In addition, the pre-supernova star dioactive cobalt-56 indicated that in the supernova. -
Spica the Blue Giant Spica Is on the Left, Venus Is the Brightest on the Bottom, with Jupiter Above
Spica the blue giant Spica is on the left, Venus is the brightest on the bottom, with Jupiter above. The constellation Virgo Spica is the brightest star in this constellation. It is the 15th brightest star in the sky and is located 260 light years from earth, which makes it one of the nearest stars to our sun. Many people throughout history have observed it including Copernicus and Hipparchus. Facts • Spica is a binary star system with the primary star at 10x the sun’s mass and 7x the sun’s radius. It puts out 12,100x the lumens as our sun, placing it in the luminosity range of a sub-giant to giant star. The magnitude reading is +1.04 with a temperature of 22,400 Kelvin. It is a flushed white helium type star. The companion is 7x the sun’s mass and has a radius 3.6x as large. The companion is main sequence. The distance between these two stars is 11 million miles. 80% of the light emitted from this area comes from Spica. Spica is also a strong source of x-rays. Spica is a binary system • There are up to 3 other components in this star system. The orbit around the barycenter, or common center of mass, is as quick as four days. The bodies are so close we cannot see them apart with our telescopes. We know this because of observations of the Doppler shift in the absorption lines of the spectra. The rotation rate of both stars is faster than their mutual orbital period. -
Types of Stars Notes
STARS QUESTION • When you think of a star, what comes to mind? WHAT IS A STAR? • Star- a fixed luminous point in the night sky that is a large, remote incandescent body. • Stars are a big ball of gas. • It is held together by its own gravity. • They are made mostly of hydrogen and helium. • The closest star to Earth is the Sun. HOW ARE STARS MADE? • Stars are born in nebulas, which are like star nurseries. • In a nebula, gravity forces gas together. • As the gas comes together, it heats up and the hydrogen in the gas starts to speed up. • Eventually, the gases form a dense, hot core. • The core is middle of the star and it provides the fuel for the star’s entire life. ARE ALL STARS THE SAME? • Just like people, stars come in different sizes and colors. • The main types of stars are: • Dwarf • Main Sequence • Giant • Super Giant • Dwarf Star- a very small stars with small mass. • The most common type of star in the DWARF STARS universe. • They burn very slowly • They live for a very long time. • Some can life for trillions of years before they run out of fuel. • They also don’t shine brightly. • Example- Proxima Centauri • Two Types: • White Dwarf • One of the hottest stars in the universe. • Red Dwarf • The coldest stars in the universe. MAIN SEQUENCE STARS • Also known as medium stars. • Our sun is a main sequence star. • They are usually yellow in color. • They have a medium temperature. • These stars typically live for about 10 billion years. -
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.