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Data for Helioseismology Testing Dali Georgobiani Michigan State University Presenting the results of Bob Stein (MSU) & Åke Nordlund (NBI, Denmark) with David Benson (Kettering University) Stanford, July 29, 2008
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Numerical Method Staggered mesh Non-linear, fully compressible, 3D, explicit Spatial differencing: 6 th order centered finite difference Time advancement: 3 rd order Runge-Kutta
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Size and Resolution Size of the domain: 96 Mm x 96 Mm x 20 Mm 1000 x 1000 x 500 grid points Grid information: dx = dy = 0.1 Mm dz = 0.012–0.075 Mm dt = 0.25 sec (saved every 60 sec)
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Boundary Conditions Density: logarithmic extrapolation on top and bottom Velocity at the top is taken to be constant at its value at the last physical point Energy (per unit mass): top – slowly evolving average, bottom – fixed energy in inflows Initialization Start from existing 12x12x9 Mm simulation Extend adiabatically to 20 Mm and relax for a solar day to develop structures Double horizontally + small fraction of stretched fluctuations to remove symmetry Relax to develop large-scale structures
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Radiation Treatment LTR Non-grey, 4 bin multigroup Equation of State Tabular EOS Includes ionization, excitation H, He, H 2, other abundant elements
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Mean Atmosphere
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Sound Speed
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Vertical Velocity at 2.5 & 8 Mm depth Boxes show domain of earlier simulations at 6, 12, 24 & 48 Mm widths.
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Vertical momentum at 0, 2, 4, 16 Mm
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Vertical momentum vs depth
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Velocity stream lines Courtesy Chris Henze (NASA)
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Finite time Lyapunov exponent (proxy for vorticity) Courtesy Bryan Green (AMTI/NASA)
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Available Datasets Website http://sha.stanford.edu/stein_simhttp://sha.stanford.edu/stein_sim (some info) Contact Bob Stein stein@pa.msu.edu (more info)stein@pa.msu.edu Simulated data are being ingested into the new SDO JSOC database Thanks to Rick Bogart for his extensive help with archiving!
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Archived Data Description 9 variables: horizontal velocities Vx, Vz, vertical velocity Vy, temperature, density, pressure, internal energy, electron density, and Each snapshot of a variable is stored in a separate file; 9 variables at each time step are combined to be retrieved together Data are in FITS format Duration 511 minutes (360 minutes recorded, WIP) A snapshot of a variable occupies approximately 2 GB of disk space First and third directions are horizontal, second direction is vertical Vertical grid is provided separately (The data will be available for retrieval soon – check with Rick)
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Another Data Set 4 hour averages, with 2 hour overlap 6 variables: horizontal velocities V x, V z, vertical velocity V y, temperature, density, and sound speed Simultaneous surface velocities Stored in the IDL SAVE format at MSU Work in progress… initial 6 variables calculated and stored, now adding internal energy E
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Units of Variables Length is in 10 8 cm = 1 Mm Time is in 10 2 s Velocities V x, V z, and V y are in 10 km/s Temperature is in K Density is in 10 -7 g/cm 3 Pressure is in 10 5 dynes/cm 2 Internal energy is in 10 5 ergs/cm 3 Electron density is log cm -3
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Data Analysis Power spectrum Tests of time-distance methods Compare the results for the simulations and the SOHO/MDI high-res observations (211.5 Mm by 211.5 Mm patch, 512 min) The following work was performed with Junwei Zhao and Alexander Kosovichev
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Power Spectra SimulationsMDI high-res data
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Power Spectra SimulationsMDI high-res data
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Power Spectra SimulationsHinode data
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Velocity Spectra
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sqrt [k P(k)]
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Time-Distance Diagram
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TD Diagrams at Various Depths
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Exploring Simulated Surface Structures Spatial filtering Spectral analysis f-mode time-distance analysis Local correlation tracking
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Large Structures
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Time-Distance Analysis
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Horizontal Flow Fields SimulationsInversions Depth range is 2-3 Mm. The longest arrow corresponds to 300 m/s
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Local Correlation Tracking Correlation coefficient Is 0.99 But velocity amplitudes are under- estimated (~1.8 times lower than in simulations)
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These simulations provide an excellent opportunity to validate various techniques, widely used in solar physics and helio- seismology for directly obtaining otherwise inaccessible properties (subsurface flows, structures etc.) On the other hand, these analysis techniques also help to examine how realistic the simulations are Conclusions
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