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Detecting Differential Rotation and Starspot Evolution on the M Dwarf GJ 1243 with Kepler James R
Western Washington University Masthead Logo Western CEDAR Physics & Astronomy College of Science and Engineering 6-20-2015 Detecting Differential Rotation and Starspot Evolution on the M Dwarf GJ 1243 with Kepler James R. A. Davenport Western Washington University, [email protected] Leslie Hebb Suzanne L. Hawley Follow this and additional works at: https://cedar.wwu.edu/physicsastronomy_facpubs Part of the Stars, Interstellar Medium and the Galaxy Commons Recommended Citation Davenport, James R. A.; Hebb, Leslie; and Hawley, Suzanne L., "Detecting Differential Rotation and Starspot Evolution on the M Dwarf GJ 1243 with Kepler" (2015). Physics & Astronomy. 16. https://cedar.wwu.edu/physicsastronomy_facpubs/16 This Article is brought to you for free and open access by the College of Science and Engineering at Western CEDAR. It has been accepted for inclusion in Physics & Astronomy by an authorized administrator of Western CEDAR. For more information, please contact [email protected]. The Astrophysical Journal, 806:212 (11pp), 2015 June 20 doi:10.1088/0004-637X/806/2/212 © 2015. The American Astronomical Society. All rights reserved. DETECTING DIFFERENTIAL ROTATION AND STARSPOT EVOLUTION ON THE M DWARF GJ 1243 WITH KEPLER James R. A. Davenport1, Leslie Hebb2, and Suzanne L. Hawley1 1 Department of Astronomy, University of Washington, Box 351580, Seattle, WA 98195, USA; [email protected] 2 Department of Physics, Hobart and William Smith Colleges, Geneva, NY 14456, USA Received 2015 March 9; accepted 2015 May 6; published 2015 June 18 ABSTRACT We present an analysis of the starspots on the active M4 dwarf GJ 1243, using 4 years of time series photometry from Kepler. -
Results of the Helsinki Magnetic Observatory 1844–1912
Annales Geophysicae (2004) 22: 1691–1704 SRef-ID: 1432-0576/ag/2004-22-1691 Annales © European Geosciences Union 2004 Geophysicae Results of the Helsinki magnetic observatory 1844–1912 H. Nevanlinna Finnish Meteorological Institute, Geophysical Research Division, P.O.Box 503, FIN-00101 Helsinki, Finland Received: 14 August 2003 – Revised: 20 October 2003 – Accepted: 20 November 2003 – Published: 8 April 2004 Abstract. The geomagnetic field declination (D) and hori- Key words. Geomagnetism and paleomagnetism (time vari- zontal component (H ) were observed visually at the Helsinki ations, diurnal to secular) – History of geophysics (planetol- magnetic observatory between 1844–1912. About 2.0 mil- ogy) – Magnetospheric physics (solar wind-magnetosphere lion single observations of the magnetic components are interactions) available. The observing equipment and observation meth- ods were the same for almost 70 years. The Helsinki data series is thus rather homogeneous and suitable for magnetic field analysis of both internal and external origin for about 1 Introduction five sunspot cycles (sunspot cycles 9–13). Due to distur- bances from nearby electric tramway traffic, most of the ob- Geomagnetic phenomena, occurring both in time and space, servations after 1897 are very noisy and unreliable for mag- were intensively studied already at the turn of the 18th and netic activity studies. Observations of D (1844–1897) have 19th centuries. The theoretical study of geomagnetism in the been converted into an absolute scale but H refers to vari- 1820s received an enormous momentum from the discov- ation values only. Observations of D have been previously ery of the electromagnetic interaction demonstrated by H. analyzed and published for the time interval 1844–1880. -
Differential Rotation of Kepler-71 Via Transit Photometry Mapping of Faculae and Starspots
MNRAS 484, 618–630 (2019) doi:10.1093/mnras/sty3474 Advance Access publication 2019 January 16 Differential rotation of Kepler-71 via transit photometry mapping of faculae and starspots Downloaded from https://academic.oup.com/mnras/article-abstract/484/1/618/5289895 by University of Southern Queensland user on 14 November 2019 S. M. Zaleski ,1‹ A. Valio,2 S. C. Marsden1 andB.D.Carter1 1University of Southern Queensland, Centre for Astrophysics, Toowoomba 4350, Australia 2Center for Radio Astronomy and Astrophysics, Mackenzie Presbyterian University, Rua da Consolac¸ao,˜ 896 Sao˜ Paulo, Brazil Accepted 2018 December 19. Received 2018 December 18; in original form 2017 November 16 ABSTRACT Knowledge of dynamo evolution in solar-type stars is limited by the difficulty of using active region monitoring to measure stellar differential rotation, a key probe of stellar dynamo physics. This paper addresses the problem by presenting the first ever measurement of stellar differential rotation for a main-sequence solar-type star using starspots and faculae to provide complementary information. Our analysis uses modelling of light curves of multiple exoplanet transits for the young solar-type star Kepler-71, utilizing archival data from the Kepler mission. We estimate the physical characteristics of starspots and faculae on Kepler-71 from the characteristic amplitude variations they produce in the transit light curves and measure differential rotation from derived longitudes. Despite the higher contrast of faculae than those in the Sun, the bright features on Kepler-71 have similar properties such as increasing contrast towards the limb and larger sizes than sunspots. Adopting a solar-type differential rotation profile (faster rotation at the equator than the poles), the results from both starspot and facula analysis indicate a rotational shear less than about 0.005 rad d−1, or a relative differential rotation less than 2 per cent, and hence almost rigid rotation. -
Space Weather
ASTRONOMY AND ASTROPHYSICS LIBRARY Series Editors: G. Börner, Garching, Germany A. Burkert, München, Germany W. B. Burton, Charlottesville, VA, USA and Leiden, The Netherlands M. A. Dopita, Canberra, Australia A. Eckart, Köln, Germany T. Encrenaz, Meudon, France E. K. Grebel, Heidelberg, Germany B. Leibundgut, Garching, Germany J. Lequeux, Paris, France A. Maeder, Sauverny, Switzerland V.Trimble, College Park, MD, and Irvine, CA, USA Kenneth R. Lang The Sun from Space Second Edition 123 Kenneth R. Lang Department of Physics and Astronomy Tufts University Medford MA 02155 USA [email protected] Cover image: Solar cycle magnetic variations. These magnetograms portray the polarity and distribution of the magnetism in the solar photosphere. They were made with the Vacuum Tower Telescope of the National Solar Observatory at Kitt Peak from 8 January 1992, at a maximum in the sunspot cycle (lower left) to 25 July 1999, well into the next maximum (lower right). Each magnetogram shows opposite polarities as darker and brighter than average tint. When the Sun is most active, the number of sunspots is at a maximum, with large bipolar sunspots that are oriented in the east–west (left–right) direction within two parallel bands. At times of low activity (top middle), there are no large sunspots and tiny magnetic fields of different magnetic polarity can be observed all over the photosphere. The haze around the images is the inner solar corona. (Courtesy of Carolus J. Schrijver, NSO, NOAO and NSF.) ISBN: 978-3-540-76952-1 e-ISBN: 978-3-540-76953-8 Library of Congress Control Number: 2008933407 c Springer-Verlag Berlin Heidelberg 2009 This work is subject to copyright. -
The Milky Way Almost Every Star We Can See in the Night Sky Belongs to Our Galaxy, the Milky Way
The Milky Way Almost every star we can see in the night sky belongs to our galaxy, the Milky Way. The Galaxy acquired this unusual name from the Romans who referred to the hazy band that stretches across the sky as the via lactia, or “milky road”. This name has stuck across many languages, such as French (voie lactee) and spanish (via lactea). Note that we use a capital G for Galaxy if we are talking about the Milky Way The Structure of the Milky Way The Milky Way appears as a light fuzzy band across the night sky, but we also see individual stars scattered in all directions. This gives us a clue to the shape of the galaxy. The Milky Way is a typical spiral or disk galaxy. It consists of a flattened disk, a central bulge and a diffuse halo. The disk consists of spiral arms in which most of the stars are located. Our sun is located in one of the spiral arms approximately two-thirds from the centre of the galaxy (8kpc). There are also globular clusters distributed around the Galaxy. In addition to the stars, the spiral arms contain dust, so that certain directions that we looked are blocked due to high interstellar extinction. This dust means we can only see about 1kpc in the visible. Components in the Milky Way The disk: contains most of the stars (in open clusters and associations) and is formed into spiral arms. The stars in the disk are mostly young. Whilst the majority of these stars are a few solar masses, the hot, young O and B type stars contribute most of the light. -
Robustness of Solar-Cycle Empirical Rules Across Different Series
Solar Physics DOI: 10.1007/•••••-•••-•••-••••-• Robustness of Solar-Cycle Empirical Rules Across Different Series Including an Updated ADF Sunspot Group Series Ilya Usoskin1,2 · Gennady Kovaltsov3 · Wilma Kiviaho1,4 © Springer •••• Abstract Empirical rules of solar cycle evolution form important observational constraints for the solar dynamo theory. This includes the Waldmeier rule re- lating the magnitude of a solar cycle to the length of its ascending phase, and the Gnevyshev–Ohl rule clustering cycles to pairs of an even-numbered cycle followed by a stronger odd-numbered cycle. These rules were established as based on the “classical” Wolf sunspot number series, which has been essentially revisited recently, with several revised sets released by the research community. Here we test the robustness of these empirical rules for different sunspot (group) series for the period 1749 – 1996, using four classical and revised international sunspot numbers and group sunspot-number series. We also provide an update of the sunspot group series based on the active-day fraction (ADF) method, using the new database of solar observations. We show that the Waldmeier rule is robust and independent of the exact sunspot (group) series: its classical and n + 1 (relating the length of n-th cycle to the magnitude of (n + 1)-th cycle) formulations are significant or highly significant for all series, while its simplified formulation (relating the magnitude of a cycle to its full length) is insignificant for all series. The Gnevyshev–Ohl rule was found robust for all analyzed series for Cycles 8 – 21, but unstable across the Dalton minimum and before it. -
Differential Rotation in Sun-Like Stars from Surface Variability and Asteroseismology
Differential rotation in Sun-like stars from surface variability and asteroseismology Dissertation zur Erlangung des mathematisch-naturwissenschaftlichen Doktorgrades “Doctor rerum naturalium” der Georg-August-Universität Göttingen im Promotionsprogramm PROPHYS der Georg-August University School of Science (GAUSS) vorgelegt von Martin Bo Nielsen aus Aarhus, Dänemark Göttingen, 2016 Betreuungsausschuss Prof. Dr. Laurent Gizon Institut für Astrophysik, Georg-August-Universität Göttingen Max-Planck-Institut für Sonnensystemforschung, Göttingen, Germany Dr. Hannah Schunker Max-Planck-Institut für Sonnensystemforschung, Göttingen, Germany Prof. Dr. Ansgar Reiners Institut für Astrophysik, Georg-August-Universität, Göttingen, Germany Mitglieder der Prüfungskommision Referent: Prof. Dr. Laurent Gizon Institut für Astrophysik, Georg-August-Universität Göttingen Max-Planck-Institut für Sonnensystemforschung, Göttingen Korreferent: Prof. Dr. Stefan Dreizler Institut für Astrophysik, Georg-August-Universität, Göttingen 2. Korreferent: Prof. Dr. William Chaplin School of Physics and Astronomy, University of Birmingham Weitere Mitglieder der Prüfungskommission: Prof. Dr. Jens Niemeyer Institut für Astrophysik, Georg-August-Universität, Göttingen PD. Dr. Olga Shishkina Max Planck Institute for Dynamics and Self-Organization Prof. Dr. Ansgar Reiners Institut für Astrophysik, Georg-August-Universität, Göttingen Prof. Dr. Andreas Tilgner Institut für Geophysik, Georg-August-Universität, Göttingen Tag der mündlichen Prüfung: 3 Contents 1 Introduction 11 1.1 Evolution of stellar rotation rates . 11 1.1.1 Rotation on the pre-main-sequence . 11 1.1.2 Main-sequence rotation . 13 1.1.2.1 Solar rotation . 15 1.1.3 Differential rotation in other stars . 17 1.1.3.1 Latitudinal differential rotation . 17 1.1.3.2 Radial differential rotation . 18 1.2 Measuring stellar rotation with Kepler ................... 19 1.2.1 Kepler photometry . -
Dynamo Processes Constrained by Solar and Stellar Observations Maria A
Long Term Datasets for the Understanding of Solar and Stellar Magnetic Cycles Proceedings IAU Symposium No. 340, 2018 c 2018 International Astronomical Union D. Banerjee, J. Jiang, K. Kusano, & S. Solanki, eds. DOI: 00.0000/X000000000000000X Dynamo Processes Constrained by Solar and Stellar Observations Maria A. Weber1,2 1Department of Astronomy and Astrophysics, University of Chicago 2Department of Astronomy, Adler Planetarium, Chicago, IL email: [email protected] Abstract. Our understanding of stellar dynamos has largely been driven by the phenomena we have observed of our own Sun. Yet, as we amass longer-term datasets for an increasing number of stars, it is clear that there is a wide variety of stellar behavior. Here we briefly review observed trends that place key constraints on the fundamental dynamo operation of solar-type stars to fully convective M dwarfs, including: starspot and sunspot patterns, various magnetism-rotation correlations, and mean field flows such as differential rotation and meridional circulation. We also comment on the current insight that simulations of dynamo action and flux emergence lend to our working knowledge of stellar dynamo theory. While the growing landscape of both observations and simulations of stellar magnetic activity work in tandem to decipher dynamo action, there are still many puzzles that we have yet to fully understand. Keywords. stars, Sun, activity, magnetic fields, interiors, observations, simulations 1. Introduction: Our Unique Dynamo Perspective Historically, our study of stellar dynamos has been shaped by observations of the Sun over a small portion of its existence. Magnetic braking facilitated through the solar wind has spun down the Sun from a likely chaotic youth to its current middle-aged state. -
Graphical Evidence for the Solar Coronal Structure During the Maunder Minimum: Comparative Study of the Total Eclipse Drawings in 1706 and 1715
J. Space Weather Space Clim. 2021, 11,1 Ó H. Hayakawa et al., Published by EDP Sciences 2021 https://doi.org/10.1051/swsc/2020035 Available online at: www.swsc-journal.org Topical Issue - Space climate: The past and future of solar activity RESEARCH ARTICLE OPEN ACCESS Graphical evidence for the solar coronal structure during the Maunder minimum: comparative study of the total eclipse drawings in 1706 and 1715 Hisashi Hayakawa1,2,3,4,*, Mike Lockwood5,*, Matthew J. Owens5, Mitsuru Sôma6, Bruno P. Besser7, and Lidia van Driel – Gesztelyi8,9,10 1 Institute for Space-Earth Environmental Research, Nagoya University, 4648601 Nagoya, Japan 2 Institute for Advanced Researches, Nagoya University, 4648601 Nagoya, Japan 3 Science and Technology Facilities Council, RAL Space, Rutherford Appleton Laboratory, Harwell Campus, OX11 0QX Didcot, UK 4 Nishina Centre, Riken, 3510198 Wako, Japan 5 Department of Meteorology, University of Reading, RG6 6BB Reading, UK 6 National Astronomical Observatory of Japan, 1818588 Mitaka, Japan 7 Space Research Institute, Austrian Academy of Sciences, 8042 Graz, Austria 8 Mullard Space Science Laboratory, University College London, RH5 6NT Dorking, UK 9 LESIA, Observatoire de Paris, Université PSL, CNRS, Sorbonne Université, Université Paris Diderot, Sorbonne Paris Cité, 92195 Meudon, France 10 Konkoly Observatory, Hungarian Academy of Sciences, 1121 Budapest, Hungary Received 18 October 2019 / Accepted 29 June 2020 Abstract – We discuss the significant implications of three eye-witness drawings of the total solar eclipse on 1706 May 12 in comparison with two on 1715 May 3, for our understanding of space climate change. These events took place just after what has been termed the “deep Maunder Minimum” but fall within the “extended Maunder Minimum” being in an interval when the sunspot numbers start to recover. -
Rotation and Stellar Evolution
EPJ Web of Conferences 43, 01005 (2013) DOI: 10.1051/epjconf/20134301005 C Owned by the authors, published by EDP Sciences, 2013 Rotation and stellar evolution P. Eggenbergera Observatoire de Genève, Université de Genève, 51 Ch. des Maillettes, 1290 Sauverny, Suisse Abstract. The effects of rotation on the evolution and properties of low-mass stars are first discussed from the pre-main sequence to the red giant phase. We then briefly indicate how some observational constraints available for these stars can help us progress in our understanding of the dynamical processes at work in stellar interiors. 1. INTRODUCTION Rotation is an important physical process that can have a significant impact on stellar evolution (see e.g. [1]). Rotational effects have generally been included in stellar evolution codes in the context of shellular rotation, which assumes that a strongly anisotropic turbulence leads to an essentially constant angular velocity on the isobars [2]. Here, we first illustrate the impact of rotation on the properties of low-mass stars at different evolutionary phases by presenting models computed with the Geneva stellar evolution code that includes a detailed treatment of shellular rotation [3]. We then compare these models to some observational constraints available for low-mass stars, which are particularly useful to constrain the modelling of the dynamical processes operating in stellar interiors. 2. EFFECTS OF ROTATION 2.1 Pre-main sequence The effects of rotation during the pre-main sequence (PMS) evolution of solar-type stars are first briefly discussed (see [4] for a more detailed discussion). Figure 1 (left) illustrates the change in the HR diagram due to rotational effects during the PMS evolution of 1 M models with a solar chemical composition and a solar-calibrated parameter for the mixing-length. -
Galactic Rotation II
1 Galactic Rotation • See SG 2.3, BM ch 3 B&T ch 2.6,2.7 B&T fig 1.3 and ch 6 • Coordinate system: define velocity vector by π,θ,z π radial velocity wrt galactic center θ motion tangential to GC with positive values in direct of galactic rotation z motion perpendicular to the plane, positive values toward North If the galaxy is axisymmetric galactic pole and in steady state then each pt • origin is the galactic center (center or in the plane has a velocity mass/rotation) corresponding to a circular • Local standard of rest (BM pg 536) velocity around center of mass • velocity of a test particle moving in of MW the plane of the MW on a closed orbit that passes thru the present position of (π,θ,z)LSR=(0,θ0,0) with 2 the sun θ0 =θ0(R) Coordinate Systems The stellar velocity vectors are z:velocity component perpendicular to plane z θ: motion tangential to GC with positive velocity in the direction of rotation radial velocity wrt to GC b π: GC π With respect to galactic coordinates l +π= (l=180,b=0) +θ= (l=30,b=0) +z= (b=90) θ 3 Local standard of rest: assume MW is axisymmetric and in steady state If this each true each point in the pane has a 'model' velocity corresponding to the circular velocity around of the center of mass. An imaginery point moving with that velocity at the position of the sun is defined to be the LSR (π,θ,z)LSR=(0,θ0,0);whereθ0 = θ0(R0) 4 Description of Galactic Rotation (S&G 2.3) • For circular motion: relative angles and velocities observing a distant point • T is the tangent point V =R sinl(V/R-V /R ) r 0 0 0 Vr Because V/R drops with R (rotation curve is ~flat); for value 0<l<90 or 270<l<360 reaches a maximum at T max So the process is to find Vr for each l and deduce V(R) =Vr+R0sinl For R>R0 : rotation curve from HI or CO is degenerate ; use masers, young stars with known distances 5 Galactic Rotation- S+G sec 2.3, B&T sec 3.2 • Consider a star in the midplane of the Galactic disk with Galactic longitude, l, at a distance d, from the Sun. -
Spectroscopic Analysis of Stellar Rotational Velocity at the Bottom of the Main Sequence
University of Pennsylvania ScholarlyCommons Publicly Accessible Penn Dissertations 2018 Spectroscopic Analysis Of Stellar Rotational Velocity At The Bottom Of The Main Sequence Steven Gilhool University of Pennsylvania, [email protected] Follow this and additional works at: https://repository.upenn.edu/edissertations Part of the Astrophysics and Astronomy Commons Recommended Citation Gilhool, Steven, "Spectroscopic Analysis Of Stellar Rotational Velocity At The Bottom Of The Main Sequence" (2018). Publicly Accessible Penn Dissertations. 3043. https://repository.upenn.edu/edissertations/3043 This paper is posted at ScholarlyCommons. https://repository.upenn.edu/edissertations/3043 For more information, please contact [email protected]. Spectroscopic Analysis Of Stellar Rotational Velocity At The Bottom Of The Main Sequence Abstract This thesis presents analyses aimed at understanding the rotational properties of stars at the bottom of the main sequence. The evolution of stellar angular momentum is intertwined with magnetic field generation, mass outflows, convective motions, and many other stellar properties and processes. This complex interplay has made a comprehensive understanding of stellar angular momentum evolution elusive. This is particularly true for low-mass stars due to the observational challenges they present. At the very bottom of the main sequence (spectral type < M4), stars become fully convective. While this ‘Transition to Complete Convection’ presents mysteries of its own, observing the rotation of stars across this boundary can provide insight into stellar structure and magnetic fields, as well as their oler in driving the evolution of stellar angular momentum. I present here a review of our understanding of rotational evolution in stars of roughly solar mass down to the end of the main sequence.