ASTRONUM-2013, July 1-5, 2013, Biarritz, France 1 2 3 - - PowerPoint PPT Presentation

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


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Yuri Omelchenko SciberQuest, San Diego, CA Collaborators:

  • H. Karimabadi, H. X. Vu (SciberQuest)

ASTRONUM-2013, July 1-5, 2013, Biarritz, France

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Bowshock/foreshock physics

Magnetosheath turbulence

Ionospheric outflow

Effect of O+ in magnetotail

Ring currents

Turbulence in the magnetotail

Transport /formation of boundaries

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Solar Wind Inflow Boundary Condition Simulation Domain 1 20 x 30 x 30 RE

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20 RE 100 RE 1 RE =130 c/ωp

Ω-1=0.5sec

1 RE =6 c/ωp

Ω-1=1.5sec

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Magnetosphere is a Multiscale Coupled System:

 Spatial scales vary from centimeters to 200 RE (span of 1011 spatial scales!)  Temporal scales vary from less than milliseconds to days (span of 108 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 (1024) and beyond
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  • 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 Q: Can we advance solution in time asynchronously in accordance with locally varying time scales?

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

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Dt 2Dt

T: CELL # 1 2 3 4 5 6 7 .. S(T) = Time-driven simulation updates the entire system Event-driven simulation updates active cells only S(0) S(Dt) S(2Dt)

update only active cells

S(0)

T1 T2

S(T1) S(T2)

update only active cells update all cells update all cells

T:

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  • 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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PIC Δt Field Δt

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t=1/Ωi t=3/Ωi t=7/Ωi

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t=1/Ωi t=3/Ωi t=7/Ωi

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t=1/Ωi t=3/Ωi t=7/Ωi

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Density Tperp Tpar

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Field Δt PIC Δt

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Load Load imbalance

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►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).

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