john santarius and greg moses university of wisconsin hapl project meeting pppl december 12-13, 2006...
TRANSCRIPT
John Santarius and Greg Moses
University of Wisconsin
HAPL Project Meeting
PPPLDecember 12-13, 2006
Effects of Long Mean-Free-PathIons 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.
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.
JFS 2006 Fusion Technology Institute, University of Wisconsin 4
For Pure Hydro Motion,Velocities Get Unphysically High
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).
JFS 2006 Fusion Technology Institute, University of Wisconsin 6
Slowest Ghost Zone Fades after a Short Time
JFS 2006 Fusion Technology Institute, University of Wisconsin 7
After a Short Time,Ghost Zones Nearly Free-Stream
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.
JFS 2006 Fusion Technology Institute, University of Wisconsin 9
Reserve Slides
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
JFS 2006 Fusion Technology Institute, University of Wisconsin 11
Qualitative Motion of Ghost and Hydro Zones Appears Reasonable