astronum 2013 july 1 5 2013 biarritz france
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ASTRONUM-2013, July 1-5, 2013, Biarritz, France 1 2 3 - PowerPoint PPT Presentation

Yuri Omelchenko SciberQuest, San Diego, CA Collaborators: H. Karimabadi, H. X. Vu (SciberQuest) ASTRONUM-2013, July 1-5, 2013, Biarritz, France 1 2 3 Bowshock/foreshock physics Magnetosheath turbulence Ionospheric outflow 4


  1. Yuri Omelchenko SciberQuest, San Diego, CA Collaborators: H. Karimabadi, H. X. Vu (SciberQuest) ASTRONUM-2013, July 1-5, 2013, Biarritz, France 1

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  4.  Bowshock/foreshock physics  Magnetosheath turbulence  Ionospheric outflow 4 Effect of O+ in magnetotail   Ring currents  Turbulence in the magnetotail  Transport /formation of boundaries

  5. Simulation Domain 3 1 20 x 30 x 30 R E Solar Wind Inflow Boundary Condition 1 R E =130 c/ ω p 1 R E =6 c/ ω p Ω -1 =0.5sec Ω -1 =1.5sec 20 R E 100 R E 5

  6. Magnetosphere is a Multiscale Coupled System:  Spatial scales vary from centimeters to 200 R E (span of 10 11 spatial scales!)  Temporal scales vary from less than milliseconds to days (span of 10 8 temporal scales!)  Electron physics: e.g., controls reconnection rate  Ion physics: e.g., accounts for formation of boundaries, transport, energization  Dynamic M-I coupling: still missing in kinetic simulations  Requires yottaflops (10 24 ) and beyond

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  8. Q: Can we advance solution in time asynchronously in accordance with locally varying time scales?  Time-Driven (Stepped) Simulation (TDS)  stability issues (for dt > CFL)  diffusion/dispersion issues (for dt < < CFL)  inactive regions are still time-stepped  local time stepping has synchronization issues Discrete-Event Simulation (DES)   updates are driven by physical changes (= > speedup)  changes are always limited (= > accuracy/stability)  arbitrary grids may be considered  adaptive synchronization via event preemption

  9. Generalized Cells have different equation: “trajectories” Event Cells have different ∆t’s scheduling:

  10. CELL # 1 2 3 4 5 6 7 .. S(T) = update all cells update all cells S(2 D t) S( D t) Time-driven simulation S(0) updates the entire system 0 D t 2D t T: update only update only active cells active cells Event-driven simulation updates active cells only S(0) S(T1) S(T2) 0 T1 T2 T:

  11. 1. For df/ dt = R schedule events: for each “state” predict Δt based on its trajectory, f(t) and accuracy threshold, Δf. 2. Update  synchronize  [preempt?]  reschedule events.

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  13. PIC Δ t Field Δ t 1 5

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  15. t=1/ Ω i t=3/ Ω i t=7/ Ω i

  16. t=1/ Ω i t=3/ Ω i t=7/ Ω i

  17. t=1/ Ω i t=3/ Ω i t=7/ Ω i

  18. T par T perp Density

  19. Field Δt PIC Δt

  20. Load Load imbalance

  21. ► Hybrid simulations are revealing new features of the solar wind interaction with the magnetosphere and laboratory plasmas. ► Disparate time scales in global 3D simulations can be addressed with DES. First parallel 3D DES runs have just been performed on 200 cpus. ► DES makes possible new advances in global hybrid simulations by enabling: (i) model coupling (e.g., I-M), (ii) new electron physics (e.g., X-Hybrid). ► DEScan be applied to MHD , CFD , PIC (turbulence, unstructured grids, higher-order methods, etc).

  22. 2006: 1D PDEs 2008: 1D Hybrid 2010: 2D Hybrid (serial) 2013: 2D/3D HYPERS (parallel) 30

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