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Marc Swisdak The Second Workshop on Thin Current Sheets April 20, 2004
The Structure of Thin Current Sheets Associated with Reconnection X-lines Marc Swisdak The Second Workshop on Thin Current Sheets April 20, 2004
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Collaborators J. Drake U. of Maryland M. Shay J. McIlhargey B. Rogers
A. Zeiler U. of Maryland UMBC Dartmouth College MPP-Garching
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z y Simulation: x J Bguide Breconn Reconnecting field: x
Inflow velocity: y Guide field/Current: z
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p3d Details Also: Relativistic PIC code Double Harris sheet
Periodic BCs Relativistic PIC code Boris algorithm for particles Trapezoidal leapfrog for fields Multigrid for Poisson’s equation MPI parallelization Biggest runs: 512x256x256 2048 processors ~109 particles How we cheat: me/mi large c/cA small
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The Point Q: At what strength does the guide field become important?
A: Bg 0.1 B0
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No Guide Field: Overview
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Development of Bifurcation
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Temperature
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Velocity Distributions
@ x-line: Beams are due to Speiser figure-8 orbits @ bifurcation: Multiple peaks from two beams
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Balancing the Reconnection Electric Field
Ideal MHD Pressure tensor Electron Inertia
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Balancing the Reconnection Electric Field
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Guide Field: Bg=1B0 Current sheet not bifurcated
Electrons magnetized at the x-line Canted separtrices E|| interacting with Bg
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Temperature, Bg=1
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Balancing the Reconnection Electric Field
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Guide Field Criterion What is the minimum Bg so that the e- excursions are less than de? Reconnection Rate:
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X-line Structure: Bg = 0, 0.2, 1
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Temperature, Bg=0.2
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Off-Diagonal Pressure Tensor, Pyz
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X-line Distribution Functions
Why is this important? Development of x-line turbulence. Why does it happen? Bg means longer acceleration times.
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Conclusions Bg ~ 0.1B0 is enough to influence the structure of x-lines. Affects: Flow geometries, separatrices, particle orbits (temperatures), particle energization, development of turbulence (?) Doesn’t affect: Reconnection rate, breaking of frozen-in condition Implication: Anti-parallel reconnection is rare in real systems. Most reconnection is component reconnection
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