Numerical Simulations of Solar Magneto-Convection

Slides:



Advertisements
Similar presentations
Particle acceleration in a turbulent electric field produced by 3D reconnection Marco Onofri University of Thessaloniki.
Advertisements

Numerical Simulations of Supergranulation and Solar Oscillations Åke Nordlund Niels Bohr Institute, Univ. of Copenhagen with Bob Stein (MSU) David Benson,
August 22, 2006IAU Symposium 239 Observing Convection in Stellar Atmospheres John Landstreet London, Canada.
Direct numerical simulation study of a turbulent stably stratified air flow above the wavy water surface. O. A. Druzhinin, Y. I. Troitskaya Institute of.
Emerging Flux Simulations Bob Stein A.Lagerfjard Å. Nordlund D. Benson D. Georgobiani 1.
Åke Nordlund & Anders Lagerfjärd Niels Bohr Institute, Copenhagen Bob Stein Dept. of Physics & Astronomy, MSU, East Lansing.
Simulation of Flux Emergence from the Convection Zone Fang Fang 1, Ward Manchester IV 1, William Abbett 2 and Bart van der Holst 1 1 Department of Atmospheric,
Design of Systems with INTERNAL CONVECTION P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi An Essential Part of Exchanging.
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.
Solar Convection Simulations Bob Stein David Benson.
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.
Atmospheric Analysis Lecture 3.
Solar Turbulence Friedrich Busse Dali Georgobiani Nagi Mansour Mark Miesch Aake Nordlund Mike Rogers Robert Stein Alan Wray.
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.
Solar Magneto-Convection: Structure & Dynamics Robert Stein - Mich. State Univ. Aake Nordlund - NBIfAFG.
Excitation of Oscillations in the Sun and Stars Bob Stein - MSU Dali Georgobiani - MSU Regner Trampedach - MSU Martin Asplund - ANU Hans-Gunther Ludwig.
Super-granulation Scale Convection Simulations Robert Stein, David Benson - Mich. State Univ. Aake Nordlund - Niels Bohr Institute.
Supergranulation-Scale Simulations of Solar Convection Robert Stein, Michigan State University, USA Aake Nordlund, Astronomical Observatory, NBIfAFG, Denmark.
SSL (UC Berkeley): Prospective Codes to Transfer to the CCMC Developers: W.P. Abbett, D.J. Bercik, G.H. Fisher, B.T. Welsch, and Y. Fan (HAO/NCAR)
Chamber Dynamic Response Modeling Zoran Dragojlovic.
Data for Helioseismology Testing Dali Georgobiani Michigan State University Presenting the results of Bob Stein (MSU) & Åke Nordlund (NBI, Denmark) with.
Solar Surface Dynamics convection & waves Bob Stein - MSU Dali Georgobiani - MSU Dave Bercik - MSU Regner Trampedach - MSU Aake Nordlund - Copenhagen Mats.
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.
Thermal Development of Internal Flows P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Concept for Precise Design ……
Ch. 5 - Basic Definitions Specific intensity/mean intensity Flux
Solar Physics Course Lecture Art Poland Modeling MHD equations And Spectroscopy.
Overview of equations and assumptions Elena Khomenko, Manuel Collados, Antonio Díaz Departamento de Astrofísica, Universidad de La Laguna and Instituto.
Energy Transport and Structure of the Solar Convection Zone James Armstrong University of Hawai’i Manoa 5/25/2004 Ph.D. Oral Examination.
R. Oran csem.engin.umich.edu SHINE 09 May 2005 Campaign Event: Introducing Turbulence Rona Oran Igor V. Sokolov Richard Frazin Ward Manchester Tamas I.
Overshoot at the base of the solar convection zone What can we learn from numerical simulations? Matthias Rempel HAO / NCAR.
Momentum Equations in a Fluid (PD) Pressure difference (Co) Coriolis Force (Fr) Friction Total Force acting on a body = mass times its acceleration (W)
Decay of a simulated bipolar field in the solar surface layers Alexander Vögler Robert H. Cameron Christoph U. Keller Manfred Schüssler Max-Planck-Institute.
Models of the 5-Minute Oscillation & their Excitation Bob Stein – Michigan State U. 1.
Convective Heat Transfer in Porous Media filled with Compressible Fluid subjected to Magnetic Field Watit Pakdee* and Bawonsak Yuwaganit Center R & D on.
Modelling photospheric magnetoconvection in the weak field regime Paul Bushby & Steve Houghton (University of Cambridge) Acknowledgements: Mike Proctor,
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.
Convection: Internal Flow ( )
Magneto-Hydrodynamic Equations Mass conservation /t = − ∇ · (u) Momentum conservation (u)/t =− ∇ ·(uu)− ∇ −g+J×B−2Ω×u− ∇ · visc Energy conservation /t.
Photospheric MHD simulation of solar pores Robert Cameron Alexander Vögler Vasily Zakharov Manfred Schüssler Max-Planck-Institut für Sonnensystemforschung.
FREE CONVECTION 7.1 Introduction Solar collectors Pipes Ducts Electronic packages Walls and windows 7.2 Features and Parameters of Free Convection (1)
Gas-kineitc MHD Numerical Scheme and Its Applications to Solar Magneto-convection Tian Chunlin Beijing 2010.Dec.3.
Emerging Flux Simulations & proto Active Regions Bob Stein – Michigan State U. A.Lagerfjärd – Copenhagen U. Å. Nordlund – Niels Bohr Inst. D. Georgobiani.
Emerging Flux Simulations & semi-Sunspots Bob Stein A.Lagerfjärd Å. Nordlund D. Georgobiani 1.
Internal Flow: Heat Transfer Correlations. Fully Developed Flow Laminar Flow in a Circular Tube: The local Nusselt number is a constant throughout the.
Non-LTE ゼミ 論文紹介「 The formation of the Hα line in the solar chromosphere 」 ① T. Anan.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Sun: Magnetic Structure Feb. 16, 2012.
Substorms: Ionospheric Manifestation of Magnetospheric Disturbances P. Song, V. M. Vasyliūnas, and J. Tu University of Massachusetts Lowell Substorms:
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.
GOAL: To understand the physics of active region decay, and the Quiet Sun network APPROACH: Use physics-based numerical models to simulate the dynamic.
THE DYNAMIC EVOLUTION OF TWISTED MAGNETIC FLUX TUBES IN A THREE-DIMENSIONALCONVECTING FLOW. II. TURBULENT PUMPING AND THE COHESION OF Ω-LOOPS.
Radiative Transfer in 3D Numerical Simulations Robert Stein Department of Physics and Astronomy Michigan State University Åke Nordlund Niels Bohr Institute.
Simulation of a self-propelled wake with small excess momentum in a stratified fluid Matthew de Stadler and Sutanu Sarkar University of California San.
GEM Student Tutorial: GGCM Modeling (MHD Backbone)
Simulations and radiative diagnostics of turbulence and wave phenomena in the magnetised solar photosphere S. Shelyag Astrophysics Research Centre Queen’s.
Chapter 8: Internal Flow
Solar Surface Magneto-Convection and Dynamo Action
Chamber Dynamic Response Modeling
GOAL: To understand the physics of active region decay, and the Quiet Sun network APPROACH: Use physics-based numerical models to simulate the dynamic.
Wave heating of the partially-ionised solar atmosphere
Helioseismic data from Emerging Flux & proto Active Region Simulations
Multi-fluid modeling of ion-neutral interactions in the solar chromosphere with ionization and recombination effects.
Earth’s Ionosphere Lecture 13
Convective Heat Transfer
Supergranule Scale Convection Simulations
Generation of Alfven Waves by Magnetic Reconnection
Presentation transcript:

Numerical Simulations of Solar Magneto-Convection Bob Stein Michigan State University East Lansing, MI, USA

Outline Equations Time Advance Spatial Derivatives Diffusion Boundary Conditions Radiation Examples

Computation Solve 3D, Compressible Realistic EOS includes ionization Conservation equations mass, momentum & internal energy Induction equation Radiative transfer equation 3D, Compressible Realistic EOS includes ionization Open boundaries Fix entropy of inflowing plasma at bottom

Equations

Centering Ez, Jz uz, Bz uy, By r , e, P Ex, Jx

Time Advance 3rd order, 2N storage, Runge-Kutta

Time Advance 3rd order, leapfrog Predictor Corrector

Spatial Derivatives 5th order

Diffusion Numerical viscosity Hyperviscous enhancement

1D Shock Tube Test

MHD Shock Tube Test

Boundary Conditions horizontally periodic vertically open Original Top Boundary Conditions

Wave Reflection Gravity wave Acoustic Wave

Original Bottom Boundary Conditions: Everywhere -- Evolve towards uniform Pressure

Original Bottom Boundary Conditions: Inflows -- Evolve toward given entropy Evolve velocity towards uniform vertical & zero net mass flux Evolve magnetic field toward given horizontal field

Characteristic Boundary Conditions Physical Conditions No Pressure drift Zero net mass flux Minimal reflected waves Entropy of inflowing material at bottom given

Characteristic z-Derivatives

Boundary Equations

Local, 1D, inviscid Characteristic Equations

Outgoing Characteristics: - Calculate di from their definitions using 1-sided derivatives Incoming Characteristics: - Impose Physical Boundary Conditions

Incoming Characteristic - No Reflected Waves Characteristic equation for incoming waves at bottom & top is So boundary condition for no reflected waves is

Incoming Characteristic - No Pressure Drift Impose condition on incoming characteristic to make Impose condition at bottom, with

Incoming characteristic - Zero net mass flux Impose condition on incoming characteristic to make So Impose the condition at the top

Incoming characteristic - Specified Entropy Impose a term on the entropy characteristic equation to make

Incoming characteristics - Horizontal velocities Impose condition horizontal velocities tend toward zero

Characteristic Magnetic Boundary Condition -- a work in progress

Physics is the time consuming part Equation of state - includes ionization and molecule formation Radiative heating and cooling - LTE, non-gray, multi-group

Energy Fluxes ionization energy 3X larger energy than thermal

Tabular Equation of State includes ionization, excitation & H2 molecule formation Lookup as function of log density & internal energy per unit mass for Log Pressure Temperature Log Opacity Source Function

Radiative Cooling & Heating Produces low entropy plasma whose buoyancy work drives convection Determines (with convection and waves) mean atmospheric structure Provides diagnostics of velocity, temperature and magnetic field Reverses p-mode intensity vs. velocity asymmetry

Energy Conservation Radiative Heating/Cooling J is average over angles of integrals along rays through entire domain

Solve Feautrier equations along rays through each grid point at the surface

Rays: 5 Through Each Surface Grid Point Interpolate source function to rays at each height

Opacity is rapidly varying function of wavelength Opacity is rapidly varying function of wavelength. Reduce number by binning like magnitudes

Simplifications Only 5 rays 4 Multi-group opacity bins Assume kL a kC

Example: 3D, Compressible Magneto-Convection

Stratified convective flow: diverging upflows, turbulent downflows Velocity arrows, temperature fluctuation image (red hot, blue cool)

Stein & Nordlund, ApJL 1989

t Z Fluid Parcels reaching the surface Radiate away their Energy and Entropy r Q E S

Entropy Green & blue are low entropy downflows, red is high entropy upflows Low entropy plasma rains down from the surface

Downflows are turbulent, upflows are more laminar. Vorticity Downflows are turbulent, upflows are more laminar.

Turbulent downdrafts

Simulation Results: B Field lines

Magnetic Field Lines, t=0.5 min

Magnetic Field Lines, t=3.5 min

Magnetic Field Lines: t=6 min

Granulation

Spectrum of granulation Simulated intensity spectrum and distribution agree with observations after smoothing with telescope+seeing point spread function.

Solar velocity spectrum MDI doppler (Hathaway) TRACE correlation tracking (Shine) MDI correlation tracking (Shine) 3-D simulations (Stein & Nordlund) v ~ k-1/3 v ~ k

Line profile with velocities. Line Profiles observed simulation Line profile without velocities. Line profile with velocities.

Average profile is combination of lines of different shifts & widths. Convection produces line shifts, changes in line widths. No microturbulence, macroturbulence. Average profile is combination of lines of different shifts & widths. average profile

Magnetic Field Strength

Both simulated and observed distributions are stretched exponentials. Field Distribution simulation observed Both simulated and observed distributions are stretched exponentials.

Acoustic Oscillations (p-modes)

Tests: Comparison with Solar Observations! Granulation Intensity Distribution Horizontal Velocity Spectrum Line Profiles Magnetic Field Distribution P-Modes

P-Mode Excitation Triangles = simulation, Squares = observations (l=0-3) Excitation decreases both at low and high frequencies

The End