The Pulse of the Sun

Total Page:16

File Type:pdf, Size:1020Kb

The Pulse of the Sun Firsthand KNOWLEDGE SOLAR SYSTEM Research The Pulse of the Sun The Sun appears to us as a calmly blazing ball of gas in the sky. In reality, it is seething inside and the entire mass vibrates like a bell. Much as geophysicists use waves caused by earthquakes to explore the structure of our planet, solar researchers use the vibrations of our star to gain insights into its interior. This is how LAURENT GIZON from the MAX PLANCK INSTITUTE FOR SOLAR SYSTEM RESEARCH in Katlenburg-Lindau studies the Sun’s magnetic field. And he wants to apply this method to distant stars, as well. n the interior of the Sun, parcels of servations of the solar surface. This Ihot gas rise to the surface, cool off is possible today thanks to a world- and descend again. Physicists call wide network of ground-based tele- this rise and fall of matter convec- scopes, and above all to the joint Eu- tion, which occurs very similarly in ropean-American space observatory a saucepan. This results in the for- SOHO, which has been recording one mation of a granular pattern that image per minute of the Sun’s sur- can be seen on the Sun. This convec- face velocity field almost without in- tion also produces sound waves that terruption since 1996. propagate through the Sun and A RICH SPECTRUM cause it to vibrate, like a clapper hits OF OSCILLATIONS a bell. Researchers working with Robert Leighton at the California In- Today we know that the five-minute stitute of Technology first discovered oscillation Leighton discovered is a this phenomenon some 40 years ago. superposition of millions of modes They registered a five-minute oscil- of oscillation of various frequencies. lation on the solar surface. The manner in which the frequencies Shortly after this observation, it and wavelengths are coupled pro- was speculated that these vibrations vides information about what kind might be caused by acoustic waves. of waves they are, and also about the German solar physicist Franz-Lud- interior structure of the Sun. Solar wig Deubner confirmed this inter- physicists study these relationships pretation with improved observa- in a power spectrum. There, the low- tions carried out in 1975, and a new ermost branch at the lowest frequen- discipline was born: helioseismology. cies corresponds to surface waves The Sun, which appears in this image from the SOHO The study of solar oscillations re- that propagate horizontally, similar satellite, looks quite peaceful. However, the arcs of light on quires long, nearly continuous ob- to those on the surface of a deep the left and right edges and the grainy surface indicate that the star that gives us life is in a constant state of turmoil. : SOHO/ESA/NASA HOTO P 48 M AXP LANCKR ESEARCH 4/2005 4/2005 M AXP LANCKR ESEARCH 49 Firsthand KNOWLEDGE SOLAR SYSTEM Research photons release a portion of their rect: contrary to what was previous- IZON WEDEN G WEDISH S , S energy in countless absorption and ly assumed, neutrinos are not mass- OYAL AURENT R re-emission events involving atoms. less. They can change “identity” on /L TOCKHOLM In the upper layers, however, which their way from the Sun to the Earth, , S ESEARCH become gradually thinner and cool- and escape detection. For the neutri- R ENTER C HYSICS OF THE P er, the behavior changes. This is no detectors on Earth, a fraction of YSTEM S OLAR S NIVERSITY where convection occurs, with gas the neutrinos is invisible. OLAR U bubbles transporting the energy. Since these initial successes, helio- S OVA FOR N One of the first triumphs of helio- seismology has made great progress. NSTITUTE FOR LBA : MPI ., I , A seismology was the finding that this Today, it is used to measure, for ex- HOTO P CIENCES outer convective envelope extends to ample, the gas motions in the solar S a depth of 0.71 solar radii, making it interior or the effect of the magnetic CHARMER ET AL possible to identify the correct model field on waves. The search for the ori- CADEMY OF A : G.B. S : G.B. of the convection zone out of many gin and variability of the solar mag- HOTO P widely differing predictions. Further- netic field is of central importance. more, the previous values for opaci- This magnetic field controls solar ties, which describe how much light activity, which varies with a period can pass through matter, had to be of about 11 years. At times of strong Cross-section of the Sun showing a mode of oscillation. The enlarged blow-out Things are particularly complex in the vicinity of sunspots. revised to reconcile the temperature activity, massive flares occur on the shows the gas flows beneath a sunspot, as identified with local helioseismology. They are exciting objects of study for helioseismologists. profile in the models with the helio- surface, and gigantic plasma clouds The Earth is depicted in the bottom right corner for size comparison. seismological data. It would not have are ejected from the outer solar at- been possible to measure opacities in mosphere, the corona, and tear number of physical parameters are laboratories on Earth, because the through the planetary system at usually low, coincided with a period inferred, such as temperature, densi- extreme conditions in the solar inte- great speed. of cold weather – the height of what ty, pressure and gas flow velocity as rior cannot be reproduced here. is now known as the Little Ice Age. FLARES PARALYZE a function of depth and heliographic Another great contribution of he- Thus, the analysis of solar magnetic ELECTRICAL NETWORKS latitude. lioseismology concerns the solar activity could have a very direct im- , MDI-SOHO/ESA/NASA : MDI-SOHO/ESA/NASA HOTO Global helioseismology can al- neutrino problem. Neutrinos are ele- Increased solar activity impacts our pact on our day-to-day lives. P ready look back on numerous suc- mentary particles that are created in planet in widely different ways. One It is not yet understood why these OSOVICHEV cesses. The standard theory of stellar great numbers by nuclear reactions or two days after a flare, a plasma eruptions occur. Physical models are : A. K HOTO structure plays a central role in mod- in the Sun’s core. They pass through cloud might collide with the Earth’s required, however, to predict “space P ern astrophysics. Stellar models not the Sun nearly unimpeded and es- magnetic field. Under certain cir- weather,” which is a subject of grow- only describe the structure of the cape into space. The standard solar cumstances, some particles can pen- ing worldwide interest, both in re- stars, but also predict how they model predicts quite accurately how etrate the magnetic cage. Then they search and in some industry sectors. evolve. These models also enable as- many of these solar neutrinos should shoot into the atmosphere and, upon It is believed that eruptions occur There are significant variations in the speed trophysicists to narrow down the age reach the Earth. Researchers were colliding with atoms and molecules, when magnetic loops above sunspots at which waves propagate below a sunspot. High wave speeds are shown in red. and chemical composition of galax- thus surprised when their instru- produce impressive northern lights. snap into a new, less energetic con- ies and the universe as a whole. The ments registered about 30 percent The high-energy particles can also figuration, releasing energy. Solar Solar waves are seen in the oscillation power Sun serves as an important test case fewer neutrinos than expected. pose a threat to astronauts, they can storms occur preferentially at the year Hale magnetic cycle. These phe- spectrum. Each branch in this diagram provides for stellar models because it is our At first, some scientists suspected damage or even completely incapac- height of the 11-year solar cycle, nomena are somehow linked to the us with a relationship between frequencies closest star and allows for very pre- that temperature and pressure in the itate satellites orbiting the Earth, and when sunspots and magnetic regions Sun’s global magnetic field. Accord- and wavelengths of solar oscillations. cise observations. Sun’s core were lower than the stan- they can interfere with radio and are larger and more numerous. At the ing to current theories, the magnetic dard model predicted. This would re- mobile communications. In extreme same time, during the course of the field originates in the outer layers of TRANSPORT OF ocean. All other branches correspond sult in the creation of fewer neutri- cases, they may cause an entire pow- cycle, sunspots preferably occur at the Sun, where convection takes SOLAR ENERGY to various overtones of the acoustic nos. This hypothesis, however, er grid to collapse. different heliographic latitudes: when place. There, matter not only rises modes of oscillation. At the longest A key issue in stellar modeling is proved to be untenable, as helioseis- There is currently a heated debate activity decreases, the spots appear and falls, but also rotates around the wavelengths, the oscillations reach how the energy in the core – where mology ultimately confirmed the about whether fluctuations in solar ever closer to the solar equator. Fur- Sun at high speeds in a well defined the deepest layers of the sun. it is released by nuclear fusion reac- standard solar model. Thus, the solu- activity will impact the climate in thermore, it is observed that sunspots way. Magnetic field lines are coupled In global helioseismology, the tions – reaches the surface. Light tion to the solar neutrino problem the long term. In Europe for in- usually occur in pairs of opposite to the solar plasma and get stretched measurements of the frequencies of particles (photons) transport the en- had to be found elsewhere.
Recommended publications
  • Atomic Diffusion in Star Models of Type Earlier Than G
    A&A 390, 611–620 (2002) Astronomy DOI: 10.1051/0004-6361:20020768 & c ESO 2002 Astrophysics Atomic diffusion in star models of type earlier than G P. Morel and F. Thevenin ´ D´epartement Cassini, UMR CNRS 6529, Observatoire de la Cˆote d’Azur, BP 4229, 06304 Nice Cedex 4, France Received 7 February 2002 / Accepted 15 May 2002 Abstract. We introduce the mixing resulting from the radiative diffusivity associated with the radiative viscosity in the calcula- tion of stellar evolution models. We find that the radiative diffusivity significantly diminishes the efficiency of the gravitational settling in the external layers of stellar models corresponding to types earlier than ≈G. The surface abundances of chemical species predicted by the models are successfully compared with the abundances determined in members of the Hyades open cluster. Our modeling depends on an efficiency parameter, which is evaluated to a value close to unity, that we calibrate in this study. Key words. diffusion – stars: abundances – stars: evolution – Hertzsprung-Russell (HR) and C-M diagrams 1. Introduction stars do not show low surface metallicities. This large helium depletion is not likely to be observed in main sequence B-stars, ff Microscopic di usion, sometimes named “atomic” or “ele- as supported by their spectral classification which is mainly ff ment” di usion, when used in the computation of models of based on the relative strength of the helium spectral lines. main sequence stars produces (see Chaboyer et al. 2001 for The large efficiency of the atomic diffusion in the outer lay- an abridged revue) a change in the surface abundances from ers results from the large temperature and pressure gradients.
    [Show full text]
  • A Bayesian Estimation of the Helioseismic Solar Age (Research Note)
    A&A 580, A130 (2015) Astronomy DOI: 10.1051/0004-6361/201526419 & c ESO 2015 Astrophysics A Bayesian estimation of the helioseismic solar age (Research Note) A. Bonanno1 and H.-E. Fröhlich2 1 INAF, Osservatorio Astrofisico di Catania, via S. Sofia, 78, 95123 Catania, Italy e-mail: [email protected] 2 Leibniz Institute for Astrophysics Potsdam (AIP), An der Sternwarte 16, 14482 Potsdam, Germany Received 27 April 2015 / Accepted 9 July 2015 ABSTRACT Context. The helioseismic determination of the solar age has been a subject of several studies because it provides us with an indepen- dent estimation of the age of the solar system. Aims. We present the Bayesian estimates of the helioseismic age of the Sun, which are determined by means of calibrated solar models that employ different equations of state and nuclear reaction rates. Methods. We use 17 frequency separation ratios r02(n) = (νn,l = 0 −νn−1,l = 2)/(νn,l = 1 −νn−1,l = 1) from 8640 days of low- BiSON frequen- cies and consider three likelihood functions that depend on the handling of the errors of these r02(n) ratios. Moreover, we employ the 2010 CODATA recommended values for Newton’s constant, solar mass, and radius to calibrate a large grid of solar models spanning a conceivable range of solar ages. Results. It is shown that the most constrained posterior distribution of the solar age for models employing Irwin EOS with NACRE reaction rates leads to t = 4.587 ± 0.007 Gyr, while models employing the Irwin EOS and Adelberger, et al. (2011, Rev.
    [Show full text]
  • X-Ray Sun SDO 4500 Angstroms: Photosphere
    ASTR 8030/3600 Stellar Astrophysics X-ray Sun SDO 4500 Angstroms: photosphere T~5000K SDO 1600 Angstroms: upper photosphere T~5x104K SDO 304 Angstroms: chromosphere T~105K SDO 171 Angstroms: quiet corona T~6x105K SDO 211 Angstroms: active corona T~2x106K SDO 94 Angstroms: flaring regions T~6x106K SDO: dark plasma (3/27/2012) SDO: solar flare (4/16/2012) SDO: coronal mass ejection (7/2/2012) Aims of the course • Introduce the equations needed to model the internal structure of stars. • Overview of how basic stellar properties are observationally measured. • Study the microphysics relevant for stars: the equation of state, the opacity, nuclear reactions. • Examine the properties of simple models for stars and consider how real models are computed. • Survey (mostly qualitatively) how stars evolve, and the endpoints of stellar evolution. Stars are relatively simple physical systems Sound speed in the sun Problem of Stellar Structure We want to determine the structure (density, temperature, energy output, pressure as a function of radius) of an isolated mass M of gas with a given composition (e.g., H, He, etc.) Known: r Unknown: Mass Density + Temperature Composition Energy Pressure Simplifying assumptions 1. No rotation à spherical symmetry ✔ For sun: rotation period at surface ~ 1 month orbital period at surface ~ few hours 2. No magnetic fields ✔ For sun: magnetic field ~ 5G, ~ 1KG in sunspots equipartition field ~ 100 MG Some neutron stars have a large fraction of their energy in B fields 3. Static ✔ For sun: convection, but no large scale variability Not valid for forming stars, pulsating stars and dying stars. 4.
    [Show full text]
  • 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
    [Show full text]
  • Magnetism, Dynamo Action and the Solar-Stellar Connection
    Living Rev. Sol. Phys. (2017) 14:4 DOI 10.1007/s41116-017-0007-8 REVIEW ARTICLE Magnetism, dynamo action and the solar-stellar connection Allan Sacha Brun1 · Matthew K. Browning2 Received: 23 August 2016 / Accepted: 28 July 2017 © The Author(s) 2017. This article is an open access publication Abstract The Sun and other stars are magnetic: magnetism pervades their interiors and affects their evolution in a variety of ways. In the Sun, both the fields themselves and their influence on other phenomena can be uncovered in exquisite detail, but these observations sample only a moment in a single star’s life. By turning to observa- tions of other stars, and to theory and simulation, we may infer other aspects of the magnetism—e.g., its dependence on stellar age, mass, or rotation rate—that would be invisible from close study of the Sun alone. Here, we review observations and theory of magnetism in the Sun and other stars, with a partial focus on the “Solar-stellar connec- tion”: i.e., ways in which studies of other stars have influenced our understanding of the Sun and vice versa. We briefly review techniques by which magnetic fields can be measured (or their presence otherwise inferred) in stars, and then highlight some key observational findings uncovered by such measurements, focusing (in many cases) on those that offer particularly direct constraints on theories of how the fields are built and maintained. We turn then to a discussion of how the fields arise in different objects: first, we summarize some essential elements of convection and dynamo theory, includ- ing a very brief discussion of mean-field theory and related concepts.
    [Show full text]
  • Stellar Structure and Evolution
    Lecture Notes on Stellar Structure and Evolution Jørgen Christensen-Dalsgaard Institut for Fysik og Astronomi, Aarhus Universitet Sixth Edition Fourth Printing March 2008 ii Preface The present notes grew out of an introductory course in stellar evolution which I have given for several years to third-year undergraduate students in physics at the University of Aarhus. The goal of the course and the notes is to show how many aspects of stellar evolution can be understood relatively simply in terms of basic physics. Apart from the intrinsic interest of the topic, the value of such a course is that it provides an illustration (within the syllabus in Aarhus, almost the first illustration) of the application of physics to “the real world” outside the laboratory. I am grateful to the students who have followed the course over the years, and to my colleague J. Madsen who has taken part in giving it, for their comments and advice; indeed, their insistent urging that I replace by a more coherent set of notes the textbook, supplemented by extensive commentary and additional notes, which was originally used in the course, is directly responsible for the existence of these notes. Additional input was provided by the students who suffered through the first edition of the notes in the Autumn of 1990. I hope that this will be a continuing process; further comments, corrections and suggestions for improvements are most welcome. I thank N. Grevesse for providing the data in Figure 14.1, and P. E. Nissen for helpful suggestions for other figures, as well as for reading and commenting on an early version of the manuscript.
    [Show full text]
  • Rotational Cherecteristics of Solar Radio Emissions
    Rotational charecteristics of solar radio emissions and IMF: A comparative study Mehul Mehta1, and Hari Om Vats2 1 VP & RPTP Science college, Vallabh Vidyanagar, 388 120, INDIA. meghdhanusha@yahoo,co.in 2 Physical Research Laboratory, Navrangpura, Ahmedabad, 380 009, INDIA. [email protected] Abstract In present work we have performed autocorrelation analysis of time series of disc integrated solar flux at 2800 MHz and daily observations of Interplanetary magnetic field (IMF) for the period of 1987 to 2010 to infer rotation period. The analysis presents a comparison between rotation periods obtained from radio emissions, a coronal feature and interplanetary magnetic field. The results show a correlation between two which indicates that IMF seems to emanate from regions of low latitudes while it is expected to originate from polar regions. 1.Introduction: The problem of solar rotation is being studied systematically since mid of 19th century. It was made clear that the Sun does not rotate like a solid body. Solar rotation is measured, mainly by two methods. One is observation of tracers like sunspots, faculae, filaments etc. and other is spectroscopic observations of Doppler shift of selected spectral lines. Each of these methods has its own limitations as pointed by Howard [1], in the review of observation and interpretation of solar rotation. In last two decades it has been shown by several groups that solar radio emissions can be used to estimate solar rotation [2,3 & 4] In this paper, we have used yet another method of inferring solar rotation using daily observations of solar radio emissions at 2800 MHz and interplanetary magnetic field (IMF).
    [Show full text]
  • The Solar Wind in Time: a Change in the Behaviour of Older Winds?
    MNRAS 000,1{11 (2017) Preprint 14 February 2018 Compiled using MNRAS LATEX style file v3.0 The solar wind in time: a change in the behaviour of older winds? D. O´ Fionnag´ain? and A. A. Vidotto School of Physics, Trinity College Dublin, College Green, Dublin 2, Ireland Accepted XXX. Received YYY; in original form ZZZ ABSTRACT In the present paper, we model the wind of solar analogues at different ages to in- vestigate the evolution of the solar wind. Recently, it has been suggested that winds of solar type stars might undergo a change in properties at old ages, whereby stars older than the Sun would be less efficient in carrying away angular momentum than what was traditionally believed. Adding to this, recent observations suggest that old solar-type stars show a break in coronal properties, with a steeper decay in X-ray lumi- nosities and temperatures at older ages. We use these X-ray observations to constrain the thermal acceleration of winds of solar analogues. Our sample is based on the stars from the `Sun in time' project with ages between 120-7000 Myr. The break in X-ray properties leads to a break in wind mass-loss rates (MÛ ) at roughly 2 Gyr, with MÛ (t < 2 Gyr) / t−0:74 and MÛ (t > 2 Gyr) / t−3:9. This steep decay in MÛ at older ages could be the reason why older stars are less efficient at carrying away angular mo- mentum, which would explain the anomalously rapid rotation observed in older stars. We also show that none of the stars in our sample would have winds dense enough to produce thermal emission above 1-2 GHz, explaining why their radio emissions have not yet been detected.
    [Show full text]
  • Solar Dynamo Wu Xuanyi Adviser: Prof
    Solar dynamo Wu Xuanyi Adviser: Prof. Yuqing Lou, Prof. Xuening Bai 2019/05/24 OUTLINE • Introduction: sunspots and solar cycle • Solar dynamo model • α Ω dynamo • Interface dynamo (Babcock-Leighton mechanism) • Flux transport dynamo • Summary −4 Observation: sunspots 1G = 10 T earliest extant record of sunspots: Book of Changes dark spots on sun (Galileo) have lower temperature with respect to surrounding life time: days to weeks Regions of intense magnetic fields : 0.1~0.3T ( the normal magnetic field of sun is ~10G; for earth, 0.5G) Often in pairs: leading and trailing sunspots Hale’s polarity law: opposite polarity from north to south hemisphere;the polarity changes each solar cycle Observation: solar cycle • Sunspot activity changes spatially and periodically • Sunspot activity has a period of ~11 years with magnetic field reversed • Solar cycle ~ 22 years Sunspot activity caused by advection/diffusion? Induction equation: Advection Diffusion B ηB Reynolds number: diffusion time scale : = 2 τd L τd Lu Rm = = B uB τa η advection time scale : = τa L • Rm of sun>>1 => advection dominated; field line frozen in the plasma flow • But, the diffusion time scale of sun ~ 10 10 years ≫ solar cycle period • Need other mechanism to explain solar activities Solar dynamo theory A solar dynamo model should… • Sustain the magnetic field • Cyclic polarity of 11year period • Equator-ward migration of sunspots and pole-ward migration of diffuse surface field • Polar field strength • Observed antisymmetric parity • … Solar dynamo model • αΩ dynamo • Interface dynamo
    [Show full text]
  • Helioseismology and Asteroseismology: Oscillations from Space
    Helioseismology and Asteroseismology: Oscillations from Space W. Dean Pesnell Project Scientist Solar Dynamics Observatory ¤ What are variable stars? ¤ How do we observe variable stars? ¤ Interpreting the observations ¤ Results from the Sun by MDI & HMI ¤ Other stars (Kepler, CoRoT, and MOST) What are Variable Stars? MASPG, College Park, MD, May 2014 Pulsating stars in the H-R diagram Variable stars cover the H-R diagram. Their periods tend to be short going to the lower left and long going toward the upper right. Many variable stars lie along a line where a resonant radiative instability called the κ-γ effect pumps the oscillation. κ-γ driving MASPG, College Park, MD, May 2014 Figures from J. Christensen-Dalsgaard Pulsating Star Classes Name log P ΔmV Comments (days) Cepheids 1.1 0.9 Radial, distance indicator RR Lyrae -0.3 0.9 Radial, distance indicator Type II Cepheids -1.0 0.6 Radial, confusers β Cephei -0.7 0.1 Multi-mode, opacity δ Scuti -1.1 <0.9 Nonradial DAV, ZZ Ceti -2.5 0.12 g modes, most common DBV, DOV -2.5 0.1 g modes 5 PNNV -2.5 0.05 g modes, very hot (Teff ~ 10 K) Sun -2.6 0.01% p modes See GCVS Variability Types at http://www.sai.msu.su/groups/cluster/gcvs/gcvs/iii/vartype.txt MASPG, College Park, MD, May 2014 What makes them oscillate? Many variants of the κ-γ effect, a resonant interaction of the oscillation with the luminosity of the star. The nuclear reactions in the convective core of massive stars may limit the maximum mass of a star.
    [Show full text]
  • Stellar Coronal Astronomy
    Stellar coronal astronomy Fabio Favata ([email protected]) Astrophysics Division of ESA’s Research and Science Support Department – P.O. Box 299, 2200 AG Noordwijk, The Netherlands Giuseppina Micela ([email protected]) INAF – Osservatorio Astronomico G. S. Vaiana – Piazza Parlamento 1, 90134 Palermo, Italy Abstract. Coronal astronomy is by now a fairly mature discipline, with a quarter century having gone by since the detection of the first stellar X-ray coronal source (Capella), and having benefitted from a series of major orbiting observing facilities. Several observational charac- teristics of coronal X-ray and EUV emission have been solidly established through extensive observations, and are by now common, almost text-book, knowledge. At the same time the implications of coronal astronomy for broader astrophysical questions (e.g. Galactic structure, stellar formation, stellar structure, etc.) have become appreciated. The interpretation of stellar coronal properties is however still often open to debate, and will need qualitatively new ob- servational data to book further progress. In the present review we try to recapitulate our view on the status of the field at the beginning of a new era, in which the high sensitivity and the high spectral resolution provided by Chandra and XMM-Newton will address new questions which were not accessible before. Keywords: Stars; X-ray; EUV; Coronae Full paper available at ftp://astro.esa.int/pub/ffavata/Papers/ssr-preprint.pdf 1 Foreword 3 2 Historical overview 4 3 Relevance of coronal
    [Show full text]
  • White Dwarfs - Degenerate Stellar Configurations
    White Dwarfs - Degenerate Stellar Configurations Austen Groener Department of Physics - Drexel University, Philadelphia, Pennsylvania 19104, USA Quantum Mechanics II May 17, 2010 Abstract The end product of low-medium mass stars is the degenerate stellar configuration called a white dwarf. Here we discuss the transition into this state thermodynamically as well as developing some intuition regarding the role of quantum mechanics in this process. I Introduction and Stellar Classification present at such high temperatures are small com- pared with the kinetic (thermal) energy of the parti- It is widely believed that the end stage of the low or cles. This assumption implies a mixture of free non- intermediate mass star is an extremely dense, highly interacting particles. One may also note that the pres- underluminous object called a white dwarf. Obser- sure of a mixture of different species of particles will vationally, these white dwarfs are abundant (∼ 6%) be the sum of the pressures exerted by each (this is in the Milky Way due to a large birthrate of their pro- where photon pressure (PRad) will come into play). genitor stars coupled with a very slow rate of cooling. Following this logic we can express the total stellar Roughly 97% of all stars will meet this fate. Given pressure as: no additional mass, the white dwarf will evolve into a cold black dwarf. PT ot = PGas + PRad = PIon + Pe− + PRad (1) In this paper I hope to introduce a qualitative de- scription of the transition from a main-sequence star At Hydrostatic Equilibrium: Pressure Gradient = (classification which aligns hydrogen fusing stars Gravitational Pressure.
    [Show full text]