Solar Convection Simulations Bob Stein David Benson.

Slides:



Advertisements
Similar presentations
Numerical Simulations of Supergranulation and Solar Oscillations Åke Nordlund Niels Bohr Institute, Univ. of Copenhagen with Bob Stein (MSU) David Benson,
Advertisements

Our Star, the Sun Chapter Eighteen.
Chapter 8 The Sun – Our Star.
Chapter 16 Modeling the solar interior The vibrating sun Neutrinos Solar atmosphere: –Photosphere –Chromosphere –Corona Sunspots Solar magnetic fields.
The Sun’s Dynamic Atmosphere Lecture 15. Guiding Questions 1.What is the temperature and density structure of the Sun’s atmosphere? Does the atmosphere.
Emerging Flux Simulations Bob Stein A.Lagerfjard Å. Nordlund D. Benson D. Georgobiani 1.
Initial Analysis of the Large-Scale Stein-Nordlund Simulations Dali Georgobiani Formerly at: Center for Turbulence Research Stanford University/ NASA Presenting.
Solar Convection: What it is & How to Calculate it. Bob Stein.
The Sun Astronomy 311 Professor Lee Carkner Lecture 23.
Supergranulation-Scale Solar Convection Simulations David Benson, Michigan State University, USA Robert Stein, Michigan State University, USA Aake Nordlund,
TIME-DISTANCE ANALYSIS OF REALISTIC SIMULATIONS OF SOLAR CONVECTION Dali Georgobiani, Junwei Zhao 1, David Benson 2, Robert Stein 2, Alexander Kosovichev.
Properties of stars during hydrogen burning Hydrogen burning is first major hydrostatic burning phase of a star: Hydrostatic equilibrium: a fluid element.
Solar Turbulence Friedrich Busse Dali Georgobiani Nagi Mansour Mark Miesch Aake Nordlund Mike Rogers Robert Stein Alan Wray.
1 Chromospheric UV oscillations depend on altitude and local magnetic field Noah S. Heller and E.J. Zita, The Evergreen State College, Olympia, WA
Data for Helioseismology Testing: Large-Scale Stein-Nordlund Simulations Dali Georgobiani Michigan State University Presenting the results of Bob Stein.
Convection Simulations Robert Stein Ake Nordlund Dali Georgobiani David Benson Werner Schafenberger.
Supergranulation Scale Solar Surface Convection Simulations Dali Georgobiani Michigan State University Presenting the results of Bob Stein (MSU) & Åke.
Solar Magneto-Convection: Structure & Dynamics Robert Stein - Mich. State Univ. Aake Nordlund - NBIfAFG.
Do magnetic waves heat the solar atmosphere? Dr. E.J. Zita The Evergreen State College Fri.30.May 2003 at Reed College NW Section.
Excitation of Oscillations in the Sun and Stars Bob Stein - MSU Dali Georgobiani - MSU Regner Trampedach - MSU Martin Asplund - ANU Hans-Gunther Ludwig.
From detailed magneto- convection simulations to modelling the convection zone-corona system Mats Carlsson Institute of Theoretical Astrophysics, University.
Super-granulation Scale Convection Simulations Robert Stein, David Benson - Mich. State Univ. Aake Nordlund - Niels Bohr Institute.
Stokes profiles Swedish 1m Solar Telescope, perfect seeing.
Radiative Transfer for Simulations of Stellar Envelope Convection By Regner Trampedach 8/19/04.
Supergranulation-Scale Simulations of Solar Convection Robert Stein, Michigan State University, USA Aake Nordlund, Astronomical Observatory, NBIfAFG, Denmark.
Data for Helioseismology Testing Dali Georgobiani Michigan State University Presenting the results of Bob Stein (MSU) & Åke Nordlund (NBI, Denmark) with.
Convection Simulation of an A-star By Regner Trampedach Mt. Stromlo Observatory, Australian National University 8/19/04.
Why does the temperature of the Sun’s atmosphere increase with height? Evidence strongly suggests that magnetic waves carry energy into the chromosphere.
Solar Surface Dynamics convection & waves Bob Stein - MSU Dali Georgobiani - MSU Dave Bercik - MSU Regner Trampedach - MSU Aake Nordlund - Copenhagen Mats.
The Sun The Sun in X-rays over several years The Sun is a star: a shining ball of gas powered by nuclear fusion. Luminosity of Sun = 4 x erg/s =
Stars II. Stellar Physics. 1.Overview of the structure of stars Still, First the Sun as an example.
Asymmetry Reversal in Solar Acoustic Modes Dali Georgobiani (1), Robert F. Stein (1), Aake Nordlund (2) 1. Physics & Astronomy Department, Michigan State.
Simulating Solar Convection Bob Stein - MSU David Benson - MSU Aake Nordlund - Copenhagen Univ. Mats Carlsson - Oslo Univ. Simulated Emergent Intensity.
Do magnetic waves heat the solar atmosphere? Dr. E.J. Zita The Evergreen State College American Geophysical Union SF, Dec.2003 This.
Interesting News… Regulus Age: a few hundred million years Mass: 3.5 solar masses Rotation Period:
Review of Lecture 4 Forms of the radiative transfer equation Conditions of radiative equilibrium Gray atmospheres –Eddington Approximation Limb darkening.
Energy Transport and Structure of the Solar Convection Zone James Armstrong University of Hawai’i Manoa 5/25/2004 Ph.D. Oral Examination.
Our Star, the Sun Chapter Eighteen. The Sun’s energy is generated by thermonuclear reactions in its core The energy released in a nuclear reaction corresponds.
Decay of a simulated bipolar field in the solar surface layers Alexander Vögler Robert H. Cameron Christoph U. Keller Manfred Schüssler Max-Planck-Institute.
Partially Ionized Plasma Effect in Dynamic Solar Atmosphere Naoki Nakamura 2015/07/05 Solar Seminar.
Models of the 5-Minute Oscillation & their Excitation Bob Stein – Michigan State U. 1.
Using Realistic MHD Simulations for Modeling and Interpretation of Quiet Sun Observations with HMI/SDO I. Kitiashvili 1,2, S. Couvidat 2 1 NASA Ames Research.
1. active prominences - solar prominences that change in a matter of hours.
The Sun – Our Star Our sun is considered an “average” star and is one of the 100 BILLION stars that make up the Milky Way galaxy. But by no MEANS does.
Magneto-Hydrodynamic Equations Mass conservation /t = − ∇ · (u) Momentum conservation (u)/t =− ∇ ·(uu)− ∇ −g+J×B−2Ω×u− ∇ · visc Energy conservation /t.
Gas-kineitc MHD Numerical Scheme and Its Applications to Solar Magneto-convection Tian Chunlin Beijing 2010.Dec.3.
Emerging Flux Simulations & semi-Sunspots Bob Stein A.Lagerfjärd Å. Nordlund D. Georgobiani 1.
Three-Dimensional Structure of the Active Region Photosphere as Revealed by High Angular Resolution B. W. Lites et al. 2004, Sol. Phys., 221, 65 Solar.
The Solar Interior NSO Solar Physics Summer School Tamara Rogers, HAO June 14, 2007
Sun Notes. Characteristics CLOSEST star to earth CLOSEST star to earth The bright star in the center is Proxima Centauri.
Organization and Evolution of Solar Magnetic Field Serena Criscuoli INAF,OAR In Collaboration with Ilaria Ermolli, Mauro Centrone, Fabrizio Giorgi and.
Shock heating by Fast/Slow MHD waves along plasma loops
Universe Tenth Edition Chapter 16 Our Star, the Sun Roger Freedman Robert Geller William Kaufmann III.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Sun: Magnetic Structure Feb. 16, 2012.
Simulations of Solar Convection Zone Nagi N. Mansour.
Solar Convection Simulations Robert Stein, David Benson - Mich. State Univ. Aake Nordlund - Niels Bohr Institute.
Simulated Solar Plages Robert Stein, David Benson - Mich. State Univ. USA Mats Carlsson - University of Oslo, NO Bart De Pontieu - Lockheed Martin Solar.
Outer Layers of the Sun Photosphere –Limb darkening –Sun spots Chromosphere Corona Prominences, flares, coronal mass ejections Reading
GOAL: To understand the physics of active region decay, and the Quiet Sun network APPROACH: Use physics-based numerical models to simulate the dynamic.
Radiative Transfer in 3D Numerical Simulations Robert Stein Department of Physics and Astronomy Michigan State University Åke Nordlund Niels Bohr Institute.
Simulations and radiative diagnostics of turbulence and wave phenomena in the magnetised solar photosphere S. Shelyag Astrophysics Research Centre Queen’s.
Numerical Simulations of Solar Magneto-Convection
The Impact of Small-Scale Magnetism on Solar Variability
WG1 – Sub-surface magnetic connections
GOAL: To understand the physics of active region decay, and the Quiet Sun network APPROACH: Use physics-based numerical models to simulate the dynamic.
Measuring the Astronomical Unit
Helioseismic data from Emerging Flux & proto Active Region Simulations
Earth Science Ch. 24 The Sun.
Measuring the Astronomical Unit
Supergranule Scale Convection Simulations
Presentation transcript:

Solar Convection Simulations Bob Stein David Benson

Solar Convection 1.Transports energy (from core nuclear reactions) through outer 1/3 of Sun 2.Drives the dynamics of the solar atmosphere 3.Generates the solar magnetic field 4.Excites the p-mode oscillations

The Simulation Code Conservative Compressible (M)HD equations LTE non-gray radiation transfer Realistic tabular EOS and opacities  No free parameters (except for resolution & diffusion model). 48 Mm 20 Mm (Developed with Danish collaborator Aake Nordlund)

Numerical Method Spatial differencing –6th-order finite difference –Staggered variables Time advancement –3rd order Runga-Kutta Parallelized –OpenMP, single parallel region –Scales linearly from processors as domain size increases

Results are used to: Understand spectral line-formation in the atmosphere Calculate the solar (and stellar) abundances Understand the excitation of solar oscillations Calibrate local helioseismic inversion methods Study magnetic flux emergence Calculate the influence of magnetic fields on observables Input to chromospheric & coronal modeling

Spectral Line Formation 1D models micro & macro-turbulence due to convective overshoot. Spatially resolved profiles

New abundance determinations Inhomogeneous T (see only cool gas), & P turb Raises atmosphere One scale height 3D atmosphere not same as 1D atmosphere (By Martin Asplund and former grad student Regner Trampedach)

Acoustic (p-mode) Oscillations Observed Simulated

P-Modes Excited by PdV work Triangles = simulation, Squares = observations (l=0-3) Excitation decreases at low frequencies because oscillation mode inertia increases and compressibility (dV) decreases. Excitation decreases at high frequencies because convective pressure fluctuations have long periods. (by former grad. students Dali Georgobiani & Regner Trampedach)

Local Helioseismology uses wave travel times through the atmosphere (by former grad. Student Dali Georgobiani)

Magnetic Flux Emergence Magnetic field lines rise up through the atmosphere and open out to space

G-band images from simulation at disk center & towards limb (by Norwegian collaborator Mats Carlsson) Notice: Hilly appearance of granules Bright points, where magnetic field is strong Striated bright walls of granules, when looking through magnetic field Dark micropore, where especially large magnetic flux

Waves: observed & simulated