Photons in the Radiative Zone: a Search for the Beginning Which Way Is Out? an A-Maz-Ing Model TEACHER GUIDE
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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. -
Structure and Energy Transport of the Solar Convection Zone A
Structure and Energy Transport of the Solar Convection Zone A DISSERTATION SUBMITTED TO THE GRADUATE DIVISION OF THE UNIVERSITY OF HAWAI'I IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY IN ASTRONOMY December 2004 By James D. Armstrong Dissertation Committee: Jeffery R. Kuhn, Chairperson Joshua E. Barnes Rolf-Peter Kudritzki Jing Li Haosheng Lin Michelle Teng © Copyright December 2004 by James Armstrong All Rights Reserved iii Acknowledgements The Ph.D. process is not a path that is taken alone. I greatly appreciate the support of my committee. In particular, Jeff Kuhn has been a friend as well as a mentor during this time. The author would also like to thank Frank Moss of the University of Missouri St. Louis. His advice has been quite helpful in making difficult decisions. Mark Rast, Haosheng Lin, and others at the HAO have assisted in obtaining data for this work. Jesper Schou provided the helioseismic rotation data. Jorgen Christiensen-Salsgaard provided the solar model. This work has been supported by NASA and the SOHOjMDI project (grant number NAG5-3077). Finally, the author would like to thank Makani for many interesting discussions. iv Abstract The solar irradiance cycle has been observed for over 30 years. This cycle has been shown to correlate with the solar magnetic cycle. Understanding the solar irradiance cycle can have broad impact on our society. The measured change in solar irradiance over the solar cycle, on order of0.1%is small, but a decrease of this size, ifmaintained over several solar cycles, would be sufficient to cause a global ice age on the earth. -
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. -
The Sun and the Solar Corona
SPACE PHYSICS ADVANCED STUDY OPTION HANDOUT The sun and the solar corona Introduction The Sun of our solar system is a typical star of intermediate size and luminosity. Its radius is about 696000 km, and it rotates with a period that increases with latitude from 25 days at the equator to 36 days at poles. For practical reasons, the period is often taken to be 27 days. Its mass is about 2 x 1030 kg, consisting mainly of hydrogen (90%) and helium (10%). The Sun emits radio waves, X-rays, and energetic particles in addition to visible light. The total energy output, solar constant, is about 3.8 x 1033 ergs/sec. For further details (and more accurate figures), see the table below. THE SOLAR INTERIOR VISIBLE SURFACE OF SUN: PHOTOSPHERE CORE: THERMONUCLEAR ENGINE RADIATIVE ZONE CONVECTIVE ZONE SCHEMATIC CONVECTION CELLS Figure 1: Schematic representation of the regions in the interior of the Sun. Physical characteristics Photospheric composition Property Value Element % mass % number Diameter 1,392,530 km Hydrogen 73.46 92.1 Radius 696,265 km Helium 24.85 7.8 Volume 1.41 x 1018 m3 Oxygen 0.77 Mass 1.9891 x 1030 kg Carbon 0.29 Solar radiation (entire Sun) 3.83 x 1023 kW Iron 0.16 Solar radiation per unit area 6.29 x 104 kW m-2 Neon 0.12 0.1 on the photosphere Solar radiation at the top of 1,368 W m-2 Nitrogen 0.09 the Earth's atmosphere Mean distance from Earth 149.60 x 106 km Silicon 0.07 Mean distance from Earth (in 214.86 Magnesium 0.05 units of solar radii) In the interior of the Sun, at the centre, nuclear reactions provide the Sun's energy. -
The Sun Visible Image of the Sun
The Sun Visible Image of the Sun •Our sole source of light and heat in the solar system •A very common star: a ggglowing ball of gas held together by its own gravity and powered by nuclear fusion at its center. Pressure (from heat caused by nuclear reactions) balances the gravitational pull towardhd the Sun’s center. This b al ance l ead s to a spherical ball of gas, called the Sun. What would happen if thlhe nuclear react ions (“burning”) stopped? Main Regions of the Sun Solar Properties Radius = 696,000 km (100 times Earth) Mass = 2x102 x 1030 kg (300,000 times Earth) Av. Density = 1410 kg/m3 Rotation Period = 24.9 days (equator) 29.8 days (poles) Surface temp = 5780 K The Moon ’s orbit around the Earth would easily fit within the Sun! Luminosity of the Sun = LSUN (Total light energy emitted per second) ~ 4 x 1026 W 100 billion one- megaton nuclear bombs every second! Solar constant: 2 LSUN 4R (energy/second/area attht the radi us of Earth’s orbit) The Solar Interior How do we know the interior “Helioseismology” structure of the Sun? •In the 1960s, it was discovered that the surface of the Sun vibra tes like a be ll •Internal pressure waves reflect off the photosphere •Analysis of the surface patterns of these waves tell us abou t the ins ide o f the Sun The Standard Solar Model Energy Transport within the Sun • Extremely hot core - ionized gas • No electrons left on atoms to capture photons - core/interior is transparent to light (radiation zone) • Temperature falls further from core - more and more non-ionized atoms capture the photons - gas becomes opaque to light in the convection zone • The low density in the photosphere makes it transparent to light - radiation takikes over again Convection CCionvection takkhes over when the gas is too opaque for radiative energy transp ort. -
Preparation of Papers for AIAA Technical Conferences
NASA – Final Report Design and Technical Study of Neutrino Detector Spacecraft Nickolas Solomey1 Wichita State University, Physics Division, Wichita, KS 67260-0032 A neutrino detector is proposed to be developed for use on a space probe in close orbit of the Sun. The detector will also be protected from radiation by a tungsten shield Sun shade, active veto array and passive cosmic shielding. With the intensity of solar neutrinos substantially greater in a close solar orbit than on the Earth only a small 250 kg detector is needed. It is expected that this detector and space probe studying the core of the Sun, its nuclear furnace and particle physics basic properties will bring new knowledge beyond what is currently possible for Earth bound solar neutrino detectors. 1. Introduction The Sun provides all of the energy that our planet needs for life and has been doing so for five billion years. Understanding our Sun and its interior is one goal of the NASA Heliophysics program. This is a very difficult task because very little makes it out of the Sun’s interior. Never- the-less within the last ten years neutrino detectors on Earth have started to make reliable detection of neutrinos from the fusion reactions in the interior of the Sun and have started to use this information to investigate the Sun’s nuclear furnace processes. Using a small detector in close solar orbit is a possible next step to expand this study, one which can provide more information that cannot be obtained by detectors situated on Earth. The Sun is located 150 billion meters from the Earth, even at this distance it is still a major source of neutrinos, as shown in the solar neutrino flux plot in Figure 1 [1]. -
198Lapj. . .243. .945G the Astrophysical Journal, 243:945-953
.945G .243. The Astrophysical Journal, 243:945-953, 1981 February 1 . © 1981. The American Astronomical Society. All rights reserved. Printed in U.S.A. 198lApJ. CONVECTION AND MAGNETIC FIELDS IN STARS D. J. Galloway High Altitude Observatory, National Center for Atmospheric Research1 AND N. O. Weiss Sacramento Peak Observatory2 Received 1980 March 10; accepted 1980 August 18 ABSTRACT Recent observations have demonstrated the unity of the study of stellar and solar magnetic fields. Results from numerical experiments on magnetoconvection are presented and used to discuss the concentration of magnetic flux into isolated ropes in the turbulent convective zones of the Sun or other late-type stars. Arguments are given for siting the solar dynamo at the base of the convective zone. Magnetic buoyancy leads to the emergence of magnetic flux in active regions, but weaker flux ropes are shredded and dispersed throughout the convective zone. The observed maximum field strengths in late-type stars should be comparable with the field (87rp)1/2 that balances the photospheric pressure. Subject headings: convection — hydrodynamics — stars: magnetic — Sun : magnetic fields I. INTRODUCTION In § II we summarize the results obtained for simplified The Sun is unique in having a magnetic field that can be models of hydromagnetic convection. The structure of mapped in detail, but magnetic activity seems to be a turbulent magnetic fields is then described in § III. standard feature of stars with deep convective envelopes. Theory and observation are brought together in § IV, Fields of 2000 gauss or more have been found in two where we discuss the formation of isolated flux tubes in late-type main sequence stars (Robinson, Worden, and the interior of the Sun. -