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Katharine K. Reeves 1, Terry G. Forbes 2, Jon Linker 3 & Zoran Mikić 3 1 Harvard-Smithsonian Center for Astrophysics 2 University of New Hampshire 3 Science Applications International Corporation Theoretical Predictions of Energy Release in CMEs and Calculations of Flare Emissions Thanks to the NSF-SHINE program for funding this work!
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Overview Main Goal: Energy dissipated in the current sheet Flare emissions Methods: 1. Analytic: loss-of- equilibrium model 2. Numerical: 2.5D MHD code (SAIC MAS) Lin & Forbes, 2000
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Equilibrium Curve Forbes & Priest, 1995
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Poynting Flux Thermalized
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Energy Release
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Effect of M A on Energy Time (s) Energy (x 10 31 ergs) M A = 0.001 M A = 0.006 M A = 0.1 Reeves & Forbes, ApJ, 2005
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Soft X-ray Telescope (SXT) Light Curves Observed Simulated Data from Reeves & Warren, ApJ, 2002 Simulated light curves from Reeves & Forbes, ApJ 2005
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Velocities and Light Curves Red curves Blue curves Background Field: 50 G Flux rope mass: 2.1 x 10 16 gm Background Field: 25 G Flux rope mass: 4.0 x 10 15 gm
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Densities in the flare loops Density Reeves, Warren & Forbes, ApJ, 2007
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Simulated Flare Images TRACE 171ÅTRACE 195Å SXT Al12SXT Be119 Reeves, et al., ApJ, 2007
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Loop-top knots and bars (e.g. Feldman, et al., 1995) Yohkoh SXTTRACE 171TRACE 195 (e.g. Doschek & Warren, 2005)
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SAIC MAS MHD model
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Density Temperature
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Energy over simulation domain shearing flux cancellation current sheet forms
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Current sheet
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Energy partition
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Energy into current sheet
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Energy flow at r0
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Energy flow at r1
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Simulated light curves
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XRT observations
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Conclusions The loss-of-equilibrium model is capable of simulating flare emissions characteristic of observations In the SAIC simulations, a higher fraction of the energy leaves the current sheet at the r1 boundary than the r0 boundary.
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Conclusions Conduction, viscous flow decrease the energy swept in to the current sheet via the Poynting flux. The bulk of the energy flow at r0 is conductive flux, which can be used as the input to multi-threaded 1D flare loop simulations, as in Reeves et al. (2007).
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