john santarius and greg moses university of wisconsin hapl project meeting pppl december 12-13, 2006...

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John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

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Page 1: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

John Santarius and Greg Moses

University of Wisconsin

HAPL Project Meeting

PPPLDecember 12-13, 2006

Effects of Long Mean-Free-PathIons on Shock Breakout

Page 2: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 2

Ghost zone

Hydro zone

Hydro zone

Hydro zone

Ghost zone

Hydro zone

Hydro zone

Hydro zone

Null zone

Ghost zone

Hydro zone

Hydro zone

Hydro zone

Null zone

Ghost zone

Hydro zone

Hydro zone

Hydro zone

Gap between hydro zones has closed; zones get

renumbered.

In original conception, ghost zone pushed hydro zones apart; absorption

can also occur.

In the Original Conceptual Picture, Long Mean-Free Path “Ghost” Zones Move through Hydro Zones

• Ghost zones transfer momentum with those hydro zones through which they pass.

Ghost zone

Hydro zone

Hydro zone

Hydro zone

Ghost zones now get renumbered.

Page 3: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 3

Zel’dovich & Raizer Shock-Breakout ProblemChosen for Code Development

• Zel’dovich & Raizer, Physics of Shock Waves and High-Temperature Hydrodynamic Phenomena, Chapter 25.

• Strong, spherical shock propagating through an exponentially falling density gradient. Analogous to ICF shock propagating through the blow-off plasma.

• Initial velocities equal zero; mass density and temperature shown below.

Page 4: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 4

For Pure Hydro Motion,Velocities Get Unphysically High

Page 5: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 5

Gap (Null Zone) between Hydro ZonesFills Quickly because of Internal Pressure

Hydro zones about to merge

• Ghost zones drag hydro zones upward in energy (and velocity).

Page 6: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 6

Slowest Ghost Zone Fades after a Short Time

Page 7: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 7

After a Short Time,Ghost Zones Nearly Free-Stream

Page 8: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 8

Status and Summary

• Mathematica® code appears to move hydro and long mean-free path (ghost) zones properly for the simple Zel’dovich and Raizer test case.

• Momentum transfer between zones also appears to be working.

• A minor zone renumbering problem remains to be addressed.

• Next step is to use initial conditions from a HAPL test problem.

Page 9: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 9

Reserve Slides

Page 10: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 10

DTCore

rshock (cm) < 0.001

rshock (cm) < 0.001

vshock (cm/s) 6.6 x 106

ni (cm-3) 1.5 x 1026

Ti (keV) 276

Te (keV) 72

Ave. charge state 1

rshock / mfp > 1000

DTCore

DT-CHShock

rshock (cm) < 0.001 0.026

rshock (cm) < 0.001 0.02

vshock (cm/s) 6.6 x 106 5.5 x 108

ni (cm-3) 1.5 x 1026 5.1 x 1024

Ti (keV) 276 86

Te (keV) 72 47

Ave. charge state 1DT 1CH 1

rshock / mfp > 1000 1.1

DTCore

DT-CHShock

CH-AuShock

rshock (cm) < 0.001 0.026 1.1

rshock (cm) < 0.001 0.02 0.004

vshock (cm/s) 6.6 x 106 5.5 x 108 8.6 x 107

ni (cm-3) 1.5 x 1026 5.1 x 1024 5.0 x 1018

Ti (keV) 276 86 2.8

Te (keV) 72 47 0.69

Ave. charge state 1DT 1CH 1

CH 1Au 36

rshock / mfp > 1000 1.1 0.001

At 34.592 ns, the DT-CH Shock Thickness andIncoming Ion Mean Free Paths Become Comparable

Page 11: John Santarius and Greg Moses University of Wisconsin HAPL Project Meeting PPPL December 12-13, 2006 Effects of Long Mean-Free-Path Ions on Shock Breakout

JFS 2006 Fusion Technology Institute, University of Wisconsin 11

Qualitative Motion of Ghost and Hydro Zones Appears Reasonable