The Sun's Dynamic Atmosphere
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THE EVOLUTION of SOLAR FLUX from 0.1 Nm to 160Μm: QUANTITATIVE ESTIMATES for PLANETARY STUDIES
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by St Andrews Research Repository The Astrophysical Journal, 757:95 (12pp), 2012 September 20 doi:10.1088/0004-637X/757/1/95 C 2012. The American Astronomical Society. All rights reserved. Printed in the U.S.A. THE EVOLUTION OF SOLAR FLUX FROM 0.1 nm TO 160 μm: QUANTITATIVE ESTIMATES FOR PLANETARY STUDIES Mark W. Claire1,2,3, John Sheets2,4, Martin Cohen5, Ignasi Ribas6, Victoria S. Meadows2, and David C. Catling7 1 School of Environmental Sciences, University of East Anglia, Norwich, UK NR4 7TJ; [email protected] 2 Virtual Planetary Laboratory and Department of Astronomy, University of Washington, Box 351580, Seattle, WA 98195, USA 3 Blue Marble Space Institute of Science, P.O. Box 85561, Seattle, WA 98145-1561, USA 4 Department of Physics & Astronomy, University of Wyoming, Box 204C, Physical Sciences, Laramie, WY 82070, USA 5 Radio Astronomy Laboratory, University of California, Berkeley, CA 94720-3411, USA 6 Institut de Ciencies` de l’Espai (CSIC-IEEC), Facultat de Ciencies,` Torre C5 parell, 2a pl, Campus UAB, E-08193 Bellaterra, Spain 7 Virtual Planetary Laboratory and Department of Earth and Space Sciences, University of Washington, Box 351310, Seattle, WA 98195, USA Received 2011 December 14; accepted 2012 August 1; published 2012 September 6 ABSTRACT Understanding changes in the solar flux over geologic time is vital for understanding the evolution of planetary atmospheres because it affects atmospheric escape and chemistry, as well as climate. We describe a numerical parameterization for wavelength-dependent changes to the non-attenuated solar flux appropriate for most times and places in the solar system. -
On the Solar Chromosphere Observed at the Limb with Hinode
The Astrophysical Journal, 719:469–473, 2010 August 10 doi:10.1088/0004-637X/719/1/469 C 2010. The American Astronomical Society. All rights reserved. Printed in the U.S.A. ON THE SOLAR CHROMOSPHERE OBSERVED AT THE LIMB WITH HINODE Philip G. Judge1 and Mats Carlsson2 1 High Altitude Observatory, National Center for Atmospheric Research, P.O. Box 3000, Boulder, CO 80307-3000, USA 2 Institute of Theoretical Astrophysics, P.O. Box 1029, Blindern, N-0315 Oslo, Norway Received 2010 March 8; accepted 2010 April 8; published 2010 July 21 ABSTRACT Broadband images in the Ca ii H line, from the Broadband Filter Imager (BFI) instrument on the Hinode spacecraft, show emission from spicules emerging from and visible right down to the observed limb. Surprisingly, little absorption of spicule light is seen along their lengths. We present formal solutions to the transfer equation for given (ad hoc) source functions, including a stratified chromosphere from which spicules emanate. The model parameters are broadly compatible with earlier studies of spicules. The visibility of Ca ii spicules down to the limb in Hinode data seems to require that spicule emission be Doppler shifted relative to the stratified atmosphere, either by supersonic turbulent or organized spicular motion. The non-spicule component of the chromosphere is almost invisible in the broadband BFI data, but we predict that it will be clearly visible in high spectral resolution data. Broadband Ca ii H limb images give the false impression that the chromosphere is dominated by spicules. Our analysis serves as a reminder that the absence of a signature can be as significant as its presence. -
Saturn — from the Outside In
Saturn — From the Outside In Saturn — From the Outside In Questions, Answers, and Cool Things to Think About Discovering Saturn:The Real Lord of the Rings Saturn — From the Outside In Although no one has ever traveled ing from Saturn’s interior. As gases in from Saturn’s atmosphere to its core, Saturn’s interior warm up, they rise scientists do have an understanding until they reach a level where the tem- of what’s there, based on their knowl- perature is cold enough to freeze them edge of natural forces, chemistry, and into particles of solid ice. Icy ammonia mathematical models. If you were able forms the outermost layer of clouds, to go deep into Saturn, here’s what you which look yellow because ammonia re- trapped in the ammonia ice particles, First, you would enter Saturn’s up- add shades of brown and other col- per atmosphere, which has super-fast ors to the clouds. Methane and water winds. In fact, winds near Saturn’s freeze at higher temperatures, so they equator (the fat middle) can reach turn to ice farther down, below the am- speeds of 1,100 miles per hour. That is monia clouds. Hydrogen and helium rise almost four times as fast as the fast- even higher than the ammonia without est hurricane winds on Earth! These freezing at all. They remain gases above winds get their energy from heat ris- the cloud tops. Saturn — From the Outside In Warm gases are continually rising in Earth’s Layers Saturn’s atmosphere, while icy particles are continually falling back down to the lower depths, where they warm up, turn to gas and rise again. -
ASTR 545 Module 2 HR Diagram 08.1.1 Spectral Classes: (A) Write out the Spectral Classes from Hottest to Coolest Stars. Broadly
ASTR 545 Module 2 HR Diagram 08.1.1 Spectral Classes: (a) Write out the spectral classes from hottest to coolest stars. Broadly speaking, what are the primary spectral features that define each class? (b) What four macroscopic properties in a stellar atmosphere predominantly govern the relative strengths of features? (c) Briefly provide a qualitative description of the physical interdependence of these quantities (hint, don’t forget about free electrons from ionized atoms). 08.1.3 Luminosity Classes: (a) For an A star, write the spectral+luminosity class for supergiant, bright giant, giant, subgiant, and main sequence star. From the HR diagram, obtain approximate luminosities for each of these A stars. (b) Compute the radius and surface gravity, log g, of each luminosity class assuming M = 3M⊙. (c) Qualitative describe how the Balmer hydrogen lines change in strength and shape with luminosity class in these A stars as a function of surface gravity. 10.1.2 Spectral Classes and Luminosity Classes: (a,b,c,d) (a) What is the single most important physical macroscopic parameter that defines the Spectral Class of a star? Write out the common Spectral Classes of stars in order of increasing value of this parameter. For one of your Spectral Classes, include the subclass (0-9). (b) Broadly speaking, what are the primary spectral features that define each Spectral Class (you are encouraged to make a small table). How/Why (physically) do each of these depend (change with) the primary macroscopic physical parameter? (c) For an A type star, write the Spectral + Luminosity Class notation for supergiant, bright giant, giant, subgiant, main sequence star, and White Dwarf. -
Formation and Evolution of a Multi-Threaded Solar Prominence
The Astrophysical Journal, 746:30 (12pp), 2012 February 10 doi:10.1088/0004-637X/746/1/30 C 2012. The American Astronomical Society. All rights reserved. Printed in the U.S.A. FORMATION AND EVOLUTION OF A MULTI-THREADED SOLAR PROMINENCE M. Luna1, J. T. Karpen2, and C. R. DeVore3 1 CRESST and Space Weather Laboratory NASA/GSFC, Greenbelt, MD 20771, USA 2 NASA/GSFC, Greenbelt, MD 20771, USA 3 Naval Research Laboratory, Washington, DC 20375, USA Received 2011 September 1; accepted 2011 November 8; published 2012 January 23 ABSTRACT We investigate the process of formation and subsequent evolution of prominence plasma in a filament channel and its overlying arcade. We construct a three-dimensional time-dependent model of an intermediate quiescent prominence suitable to be compared with observations. We combine the magnetic field structure of a three-dimensional sheared double arcade with one-dimensional independent simulations of many selected flux tubes, in which the thermal nonequilibrium process governs the plasma evolution. We have found that the condensations in the corona can be divided into two populations: threads and blobs. Threads are massive condensations that linger in the flux tube dips. Blobs are ubiquitous small condensations that are produced throughout the filament and overlying arcade magnetic structure, and rapidly fall to the chromosphere. The threads are the principal contributors to the total mass, whereas the blob contribution is small. The total prominence mass is in agreement with observations, assuming reasonable filling factors of order 0.001 and a fixed number of threads. The motion of the threads is basically horizontal, while blobs move in all directions along the field. -
Why Is the Corona Hotter Than It Has Any Right to Be?
Why is the corona hotter than it has any right to be? Sam Van Kooten CU Boulder SHINE 2019 Student Day Thanks to Steve Cranmer for some slides Why the Sun is the way it is The Sun is magnetically active The Sun rotates differentially Rotation + plasma = magnetism Magnetism + rotation = solar activity That’s why the Sun is the way it is Temperature Profile of the Solar Atmosphere Photosphere (top of the convection zone) Chromosphere (forest of complex structures) Corona (magnetic domination & heating conundrum) Coronal Heating ● How do you achieve those temperatures? ● Step 1: Have energy ● Step 2: Move energy ● Step 3: Turn energy to heat ● Step 4: Retain heat ● Step 5: HOT Step 1: Have energy ● The photosphere’s kinetic energy is enough by orders of magnitude Photospheric granulation Photospheric granulation Step 2: Move energy “DC” field-line braiding → “nanoflares” “AC” MHD waves “Taylor relaxation” “IR” (twist wants to untwist, due to mag. tension) Step 3: Turn energy to heat ● Turbulence ¯\_( )_/¯ ツ Step 4: Retain heat ● Very hot → complete ionization → no blackbody radiation → very limited cooling ● Combined with low density, required heat isn’t too mind-boggling Step 5: HOT So what’s the “coronal heating problem”? Cranmer & Winebarger (2019) So what’s the “coronal heating problem”? ● The theory side is fine ● All coronal heating models occur at small scales in thin plasmas – Really hard to see! ● It’s an observational problem – Can’t observe heating happening – Can’t measure or rule out models So why is the corona hotter than it -
STELLAR SPECTRA A. Basic Line Formation
STELLAR SPECTRA A. Basic Line Formation R.J. Rutten Sterrekundig Instituut Utrecht February 6, 2007 Copyright c 1999 Robert J. Rutten, Sterrekundig Instuut Utrecht, The Netherlands. Copying permitted exclusively for non-commercial educational purposes. Contents Introduction 1 1 Spectral classification (“Annie Cannon”) 3 1.1 Stellar spectra morphology . 3 1.2 Data acquisition and spectral classification . 3 1.3 Introduction to IDL . 4 1.4 Introduction to LaTeX . 4 2 Saha-Boltzmann calibration of the Harvard sequence (“Cecilia Payne”) 7 2.1 Payne’s line strength diagram . 7 2.2 The Boltzmann and Saha laws . 8 2.3 Schadee’s tables for schadeenium . 12 2.4 Saha-Boltzmann populations of schadeenium . 14 2.5 Payne curves for schadeenium . 17 2.6 Discussion . 19 2.7 Saha-Boltzmann populations of hydrogen . 19 2.8 Solar Ca+ K versus Hα: line strength . 21 2.9 Solar Ca+ K versus Hα: temperature sensitivity . 24 2.10 Hot stars versus cool stars . 24 3 Fraunhofer line strengths and the curve of growth (“Marcel Minnaert”) 27 3.1 The Planck law . 27 3.2 Radiation through an isothermal layer . 29 3.3 Spectral lines from a solar reversing layer . 30 3.4 The equivalent width of spectral lines . 33 3.5 The curve of growth . 35 Epilogue 37 References 38 Text available at \tthttp://www.astro.uu.nl/~rutten/education/rjr-material/ssa (or via “Rob Rutten” in Google). Introduction These three exercises concern the appearance and nature of spectral lines in stellar spectra. Stellar spectrometry laid the foundation of astrophysics in the hands of: – Wollaston (1802): first observation of spectral lines in sunlight; – Fraunhofer (1814–1823): rediscovery of spectral lines in sunlight (“Fraunhofer lines”); their first systematic inventory. -
Arxiv:1110.1805V1 [Astro-Ph.SR] 9 Oct 2011 Htte Olpet Ukaclrt H Lcrn,Rapid Emissions
Noname manuscript No. (will be inserted by the editor) Energy Release and Particle Acceleration in Flares: Summary and Future Prospects R. P. Lin1,2 the date of receipt and acceptance should be inserted later Abstract RHESSI measurements relevant to the fundamental processes of energy release and particle acceleration in flares are summarized. RHESSI's precise measurements of hard X-ray continuum spectra enable model-independent deconvolution to obtain the parent elec- tron spectrum. Taking into account the effects of albedo, these show that the low energy cut- < off to the electron power-law spectrum is typically ∼tens of keV, confirming that the accel- erated electrons contain a large fraction of the energy released in flares. RHESSI has detected a high coronal hard X-ray source that is filled with accelerated electrons whose energy den- sity is comparable to the magnetic-field energy density. This suggests an efficient conversion of energy, previously stored in the magnetic field, into the bulk acceleration of electrons. A new, collisionless (Hall) magnetic reconnection process has been identified through theory and simulations, and directly observed in space and in the laboratory; it should occur in the solar corona as well, with a reconnection rate fast enough for the energy release in flares. The reconnection process could result in the formation of multiple elongated magnetic islands, that then collapse to bulk-accelerate the electrons, rapidly enough to produce the observed hard X-ray emissions. RHESSI's pioneering γ-ray line imaging of energetic ions, revealing footpoints straddling a flare loop arcade, has provided strong evidence that ion acceleration is also related to magnetic reconnection. -
Spectral Classification and HR Diagram of Pre-Main Sequence Stars in NGC 6530
A&A 546, A9 (2012) Astronomy DOI: 10.1051/0004-6361/201219853 & c ESO 2012 Astrophysics Spectral classification and HR diagram of pre-main sequence stars in NGC 6530,, L. Prisinzano, G. Micela, S. Sciortino, L. Affer, and F. Damiani INAF – Osservatorio Astronomico di Palermo, Piazza del Parlamento, Italy 1, 90134 Palermo, Italy e-mail: [email protected] Received 20 June 2012 / Accepted 3 August 2012 ABSTRACT Context. Mechanisms involved in the star formation process and in particular the duration of the different phases of the cloud contrac- tion are not yet fully understood. Photometric data alone suggest that objects coexist in the young cluster NGC 6530 with ages from ∼1 Myr up to 10 Myr. Aims. We want to derive accurate stellar parameters and, in particular, stellar ages to be able to constrain a possible age spread in the star-forming region NGC 6530. Methods. We used low-resolution spectra taken with VLT/VIMOS and literature spectra of standard stars to derive spectral types of a subsample of 94 candidate members of this cluster. Results. We assign spectral types to 86 of the 88 confirmed cluster members and derive individual reddenings. Our data are better fitted by the anomalous reddening law with RV = 5. We confirm the presence of strong differential reddening in this region. We derive fundamental stellar parameters, such as effective temperatures, photospheric colors, luminosities, masses, and ages for 78 members, while for the remaining 8 YSOs we cannot determine the interstellar absorption, since they are likely accretors, and their V − I colors are bluer than their intrinsic colors. -
Multi-Spacecraft Analysis of the Solar Coronal Plasma
Multi-spacecraft analysis of the solar coronal plasma Von der Fakultät für Elektrotechnik, Informationstechnik, Physik der Technischen Universität Carolo-Wilhelmina zu Braunschweig zur Erlangung des Grades einer Doktorin der Naturwissenschaften (Dr. rer. nat.) genehmigte Dissertation von Iulia Ana Maria Chifu aus Bukarest, Rumänien eingereicht am: 11.02.2015 Disputation am: 07.05.2015 1. Referent: Prof. Dr. Sami K. Solanki 2. Referent: Prof. Dr. Karl-Heinz Glassmeier Druckjahr: 2016 Bibliografische Information der Deutschen Nationalbibliothek Die Deutsche Nationalbibliothek verzeichnet diese Publikation in der Deutschen Nationalbibliografie; detaillierte bibliografische Daten sind im Internet über http://dnb.d-nb.de abrufbar. Dissertation an der Technischen Universität Braunschweig, Fakultät für Elektrotechnik, Informationstechnik, Physik ISBN uni-edition GmbH 2016 http://www.uni-edition.de © Iulia Ana Maria Chifu This work is distributed under a Creative Commons Attribution 3.0 License Printed in Germany Vorveröffentlichung der Dissertation Teilergebnisse aus dieser Arbeit wurden mit Genehmigung der Fakultät für Elektrotech- nik, Informationstechnik, Physik, vertreten durch den Mentor der Arbeit, in folgenden Beiträgen vorab veröffentlicht: Publikationen • Mierla, M., Chifu, I., Inhester, B., Rodriguez, L., Zhukov, A., 2011, Low polarised emission from the core of coronal mass ejections, Astronomy and Astrophysics, 530, L1 • Chifu, I., Inhester, B., Mierla, M., Chifu, V., Wiegelmann, T., 2012, First 4D Recon- struction of an Eruptive Prominence -
Three-Dimensional Convective Velocity Fields in the Solar Photosphere
Three-dimensional convective velocity fields in the solar photosphere 太陽光球大気における3次元対流速度場 Takayoshi OBA Doctor of Philosophy Department of Space and Astronautical Science, School of Physical sciences, SOKENDAI (The Graduate University for Advanced Studies) submitted 2018 January 10 3 Abstract The solar photosphere is well-defined as the solar surface layer, covered by enormous number of bright rice-grain-like spot called granule and the surrounding dark lane called intergranular lane, which is a visible manifestation of convection. A simple scenario of the granulation is as follows. Hot gas parcel rises to the surface owing to an upward buoyant force and forms a bright granule. The parcel decreases its temperature through the radiation emitted to the space and its density increases to satisfy the pressure balance with the surrounding. The resulting negative buoyant force works on the parcel to return back into the subsurface, forming a dark intergranular lane. The enormous amount of the kinetic energy deposited in the granulation is responsible for various kinds of astrophysical phenomena, e.g., heating the outer atmospheres (the chromosphere and the corona). To disentangle such granulation-driven phenomena, an essential step is to understand the three-dimensional convective structure by improving our current understanding, such as the above-mentioned simple scenario. Unfortunately, our current observational access is severely limited and is far from that objective, leaving open questions related to vertical and horizontal flows in the granula- tion, respectively. The first issue is several discrepancies in the vertical flows derived from the observation and numerical simulation. Past observational studies reported a typical magnitude relation, e.g., stronger upflow and weaker downflow, with typical amplitude of ≈ 1 km/s. -
Solar Prominence Magnetic Configurations Derived Numerically
A&A 371, 328–332 (2001) Astronomy DOI: 10.1051/0004-6361:20010315 & c ESO 2001 Astrophysics Solar prominence magnetic configurations derived numerically from convection I. McKaig? Department of Mathematics, Tidewater Community College, Virginia Beach, VA 23456, USA Received 19 January 2001 / Accepted 28 February 2001 Abstract. The solar convection zone may be a mechanism for generating the magnetic fields in the corona that create and thermally insulate quiescent prominences. This connection is examined here by numerically solving a diffusion equation with convection (below the photosphere) matched to Laplace’s equation (modeling the current free corona above the photosphere). The types of fields formed resemble both Kippenhahn-Schl¨uter and Kuperus- Raadu configurations with feet that drop into supergranule boundaries. Key words. supergranulation – convection – prominences 1. Prominence models Marvelous photographs of these magnificent structures can also be found on the internet – see for example The atmosphere of the Sun, from the base of the chro- http://mesola.obspm.fr (a site run by INSU/CNRS mosphere through the corona, is structured by magnetic France) and http://sohowww.estec.esa.nl (the web fields. Presumably generated in the convection zone these site of the Solar and Heliospheric Observatory). fields break through the photosphere stimulating a vari- The field lines in the models by KS and KR are line tied ety of plasma formations, from small fibrils that outline to the photosphere (see McKaig 2001). In a previous paper convection cells to gigantic solar quiescent prominences (McKaig 2001) photospheric motions were simulated by that tower above the surface. In this paper we attempt a one-dimensional boundary condition and KS/KR type a connection between the ejection of magnetism by con- fields were obtained in the corona.