Asteroseismology of Sun-like Stars

Slides:



Advertisements
Similar presentations
Items for Teachers to Prepare for the HSPE Quality Test Preparation DOK Levels Item Specs State Standards.
Advertisements

PLAnetary Transits and Oscillations of stars H. Rauer 1, C. Catala 2, D. Pollacco 3, S. Udry 4 and the PLATO Team 1: Institut für Planetenforschung, DLR.
Stellar Atmospheres: Hydrostatic Equilibrium 1 Hydrostatic Equilibrium Particle conservation.
Asymptotic Giant Branch. Learning outcomes Evolution and internal structure of low mass stars from the core He burning phase to the tip of the AGB Nucleosynthesis.
Genetic Algorithms By: Anna Scheuler and Aaron Smittle.
On the Genetic Evolution of a Perfect Tic-Tac-Toe Strategy
Solar-like Oscillations in Red Giant Stars Olga Moreira BAG.
Asteroseismology of solar-type stars Revolutionizing the study of solar-type stars Hans Kjeldsen, Aarhus University.
A ground-based velocity campaign on Procyon Tim Bedding (Univ. Sydney) and about 50 others.
Observational properties of pulsating subdwarf B stars. Mike Reed Missouri State University With help from many, including Andrzej Baran, Staszek Zola,
Reaching the 1% accuracy level on stellar mass and radius determinations from asteroseismology Valerie Van Grootel (University of Liege) S. Charpinet (IRAP.
Exoplanet- Asteroseismology Synergies Bill Chaplin, School of Physics & Astronomy University of Birmingham, UK EAHS2012, Oxford, 2012 March 15.
Constraining Astronomical Populations with Truncated Data Sets Brandon C. Kelly (CfA, Hubble Fellow, 6/11/2015Brandon C. Kelly,
Properties of stars during hydrogen burning Hydrogen burning is first major hydrostatic burning phase of a star: Hydrostatic equilibrium: a fluid element.
Nonlinear and Non-Gaussian Estimation with A Focus on Particle Filters Prasanth Jeevan Mary Knox May 12, 2006.
Variable Stars: Pulsation, Evolution and application to Cosmology. Shashi M. Kanbur SUNY Oswego, July 2007.
Trivial Parallelization of an Existing EA Asher Freese CS401.
ASTEROSEISMOLOGY CoRoT session, January 13, 2007 Jadwiga Daszyńska-Daszkiewicz Instytut Astronomiczny, Uniwersytet Wrocławski.
PARALLEL GENETIC ALGORITHMS AND THE SCIENCE OF ASTEROSEISMOLOGY A Review of the Doctoral Dissertation Research of Dr. Travis Metcalfe.
Inversion of rotation profile for solar-like stars Jérémie Lochard IAS 19/11/04.
Catania 09/08SIAMOIS1/26 Benoît Mosser, for the SIAMOIS team Ground-based Doppler asteroseismology after CoRoT and Kepler.
GONG SoHO 24 A new era of seismology of the Sun and solar-like stars Aix-en-Provence, France Sarbani Basu Yale Unoversity.
Marc Pinsonneault (OSU).  New Era in Astronomy  Seismology  Large Surveys  We can now measure things which have been assumed in stellar modeling 
Nonradial Oscillations. The Science Case:  Stellar Ages - directly for individual stars  Age determination is direct and reliable  Ages to stars which.
PLAnetary Transits and Oscillations of stars Thierry Appourchaux for the PLATO Consortium
C/O abundance in white dwarf interior The asteroseismological data Need higher 12 C+a ? Different convective schemes The effect of 12 C+a So what?
Genetic Algorithm What is a genetic algorithm? “Genetic Algorithms are defined as global optimization procedures that use an analogy of genetic evolution.
Science Olympiad Solar System Div B 2007 Joshua Haislip.
IFAC Control of Distributed Parameter Systems, July 20-24, 2009, Toulouse Inverse method for pyrolysable and ablative materials with optimal control formulation.
1 Hybrid methods for solving large-scale parameter estimation problems Carlos A. Quintero 1 Miguel Argáez 1 Hector Klie 2 Leticia Velázquez 1 Mary Wheeler.
1 Paper Review for ENGG6140 Memetic Algorithms By: Jin Zeng Shaun Wang School of Engineering University of Guelph Mar. 18, 2002.
Future of asteroseismology II Jørgen Christensen-Dalsgaard Institut for Fysik og Astronomi, Aarhus Universitet Dansk AsteroSeismologisk Center.
Scientific aspects of SONG Jørgen Christensen-Dalsgaard Department of Physics and Astronomy Aarhus University.
The Real Music of the Spheres
Stellar Parameters through Analysis of the Kepler Oscillation Data Chen Jiang & Biwei Jiang Department of Astronomy Beijing Normal University 2 April 2010.
Boltzmann Machine (BM) (§6.4) Hopfield model + hidden nodes + simulated annealing BM Architecture –a set of visible nodes: nodes can be accessed from outside.
Excitation and damping of oscillation modes in red-giant stars Marc-Antoine Dupret, Université de Liège, Belgium Workshop Red giants as probes of the structure.
Searching for Brown Dwarf Companions to Nearby Stars Michael W. McElwain, James E. Larkin & Adam J. Burgasser (UC Los Angeles) Background on Brown Dwarfs.
Travis Metcalfe (NCAR) Asteroseismology with the Kepler Mission We are the stars which sing, We sing with our light; We are the birds of fire, We fly over.
A tool to simulate COROT light-curves R. Samadi 1 & F. Baudin 2 1 : LESIA, Observatory of Paris/Meudon 2 : IAS, Orsay.
Applications of Genetic Algorithms TJHSST Computer Systems Lab By Mary Linnell.
SOUND Chapter Twenty-Four: Sound  24.1 Properties of Sound  24.2 Sound Waves  24.3 Sound Perception and Music.
Asteroseismology A brief Introduction
1 Effect of Spatial Locality on An Evolutionary Algorithm for Multimodal Optimization EvoNum 2010 Ka-Chun Wong, Kwong-Sak Leung, and Man-Hon Wong Department.
Biologically inspired algorithms BY: Andy Garrett YE Ziyu.
PHYSICS UNDER THE BONNET OF A STELLAR EVOLUTION CODE Richard J. Stancliffe Argelander Institut für Astronomie, Universität Bonn.
Travis Metcalfe Space Science Institute + Stellar Astrophysics Centre Probing Stellar Activity with Kepler.
1. Short Introduction 1.1 Overview of helioseismology results and prospects.
Travis Metcalfe (NCAR) First results from the Asteroseismic Modeling Portal Collaborators: Michaël Bazot, Tim Bedding, Alfio Bonanno, Isa Brandão, Bill.
Subdwarf B stars from He white dwarf mergers Haili Hu.
Internal dynamics from asteroseismology for two sdB pulsators residing in close binary systems Valérie Van Grootel (Laboratoire d’Astrophysique de Toulouse.
Investigating the Low- Mass Stellar Initial Mass Function in Draco Soroush Sotoudeh (University of Minnesota) Daniel Weisz, Andrew Dolphin, Evan Skillman.
Genetic Algorithm(GA)
Hirophysics.com The Genetic Algorithm vs. Simulated Annealing Charles Barnes PHY 327.
Doppler imaging study of starspots and stellar non-radial pulsation using SONG network Sheng-hong Gu NAOC/Yunnan Observatory, Kunming, China
The Future of White Dwarf Asteroseismology Travis Metcalfe (NCAR) NGC 1514 – Crystal Ball Nebula.
CEng 713, Evolutionary Computation, Lecture Notes parallel Evolutionary Computation.
Machine Learning Supervised Learning Classification and Regression
Asteroseismology of Kepler
Asteroseismic Modeling Portal (AMP) Development
Balancing of Parallel Two-Sided Assembly Lines via a GA based Approach
C.-S. Shieh, EC, KUAS, Taiwan
Announcements HW4 due today (11:59pm) HW5 out today (due 11/17 11:59pm)
An asteroseismic data-interpretation pipeline for Kepler
A Pulsational Mechanism for Producing Keplerian Disks around Rapidly Rotating Stars Steven R. Cranmer Harvard-Smithsonian CfA.
Boltzmann Machine (BM) (§6.4)
Ay 123 Lecture 9 - Helioseismology
Applications of Genetic Algorithms TJHSST Computer Systems Lab
The SMARTS Southern HK Project
Presentation transcript:

Asteroseismology of Sun-like Stars Travis Metcalfe (HAO)

The Internal Constitution of the Stars “At first sight it would seem that the deep interior of the sun and stars is less accessible to scientific investigation than any other region of the universe. Our telescopes may probe farther and farther into the depths of space; but how can we ever obtain certain knowledge of that which is hidden behind substantial barriers? What appliance can pierce through the outer layers of a star and test the conditions within?” (written in 1926) Sir Arthur Eddington (1882 – 1944)

Seismology: seeing with sound Convection creates acoustic noise – some of it resonates

Motivation New opportunities to probe the fundamental physics of solar and stellar models. Understanding the solar structure and evolution in a broader physical context.

1D oscillations: violin strings Fundamental Third overtone First overtone Second overtone

2D oscillations: drums Radial modes Non-radial modes

2D oscillations: drums Radial modes Non-radial modes

3D oscillations: stars Radial modes Non-radial modes

3D oscillations: stars Radial modes Non-radial modes

Pulsations cause variations in spectral lines and brightness Observations Pulsations cause variations in spectral lines and brightness

Space missions will soon revolutionize the observations

Space missions will soon revolutionize the observations

Space missions will soon revolutionize the observations

Matching models to observations is an optimization problem Epistemology Matching models to observations is an optimization problem

Optimization Easy

Optimization Hard

Evolution as optimization “Evolution is cleverer than you are.” – Francis Crick

Evolution as optimization “Evolution is cleverer than you are.” – Francis Crick

Genetic algorithms Generate N random trial sets of parameter values. Evaluate the model for each trial and calculate the variance. Assign a “fitness” to each trial, inversely proportional to the variance. Select a new population from the old one, weighted by the fitness. Encode-Breed-Mutate-Decode Loop to step 2 until the solution converges.

Evolutionary operators

Parallel computing Genetic algorithms are intrinsically parallelizable Each iteration typically has 128 model evaluations Number of processors sets the number of models that can be evaluated in parallel Also need multiple runs with different random initialization

Stellar parameters Total Mass Surface Temperature Chemical composition Convective efficiency Internal chemical gradients Rotation rate Age / Evolutionary status

The Future: Eddington et al. 2007 and beyond: a flood of unprecedented observations