One-dimensional radiation-hydrodynamic scaling studies of imploding spherical plasma liners

被引:25
作者
Awe, T. J. [1 ]
Adams, C. S. [1 ]
Davis, J. S. [1 ]
Hanna, D. S. [1 ]
Hsu, S. C. [1 ]
Cassibry, J. T. [2 ]
机构
[1] Los Alamos Natl Lab, Div Phys, Los Alamos, NM 87545 USA
[2] Univ Alabama, Prop Res Ctr, Huntsville, AL 35899 USA
关键词
FUSION;
D O I
10.1063/1.3610374
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
One-dimensional radiation-hydrodynamic simulations are performed to develop insight into the scaling of stagnation pressure with initial conditions of an imploding spherical plasma shell or "liner." Simulations reveal the evolution of high-Mach-number (M), annular, spherical plasma flows during convergence, stagnation, shock formation, and disassembly, and indicate that cm-and mu s-scale plasmas with peak pressures near 1 Mbar can be generated by liners with initial kinetic energy of several hundred kilo-joules. It is shown that radiation transport and thermal conduction must be included to avoid non-physical plasma temperatures at the origin which artificially limit liner convergence and, thus, the peak stagnation pressure. Scalings of the stagnated plasma lifetime (tau(stag)) and average stagnation pressure (P-stag, the pressure at the origin, averaged over tau(stag)) are determined by evaluating a wide range of liner initial conditions. For high-M flows, tau(stag) similar to Delta R/v(0), where Delta R and v(0) are the initial liner thickness and velocity, respectively. Furthermore, for argon liners, P-stag scales approximately as v(0)(15/4) over a wide range of initial densities (n(0)) and as n(0)(1/2) over a wide range of v(0). The approximate scaling P-stag similar to M-3/2 is also found for a wide range of liner-plasma initial conditions. (C) 2011 American Institute of Physics. [doi: 10.1063/1.3610374]
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页数:11
相关论文
共 17 条
[1]  
Cassibry J. T., 2010, B AM PHYS SOC, V55, P359
[2]   Ignition scaling laws and their application to capsule design [J].
Herrmann, MC ;
Tabak, M ;
Lindl, JD .
PHYSICS OF PLASMAS, 2001, 8 (05) :2296-2304
[3]  
Hsu S. C., 2010, B AM PHYS SOC, V55, P357
[4]   Using pulsed power for hydrodynamic code validation [J].
Kanzleiter, RJ ;
Atchison, WL ;
Bowers, RL ;
Fortson, RL ;
Guzik, JA ;
Olson, RT ;
Stokes, JL ;
Turchi, PJ .
IEEE TRANSACTIONS ON PLASMA SCIENCE, 2002, 30 (05) :1755-1763
[5]   Stagnation pressure of imploding shells and ignition energy scaling of inertial confinement fusion targets [J].
Kemp, A ;
Meyer-ter-Vehn, J ;
Atzeni, S .
PHYSICAL REVIEW LETTERS, 2001, 86 (15) :3336-3339
[6]   MAGNETIZED TARGET FUSION - AN OVERVIEW [J].
KIRKPATRICK, RC ;
LINDEMUTH, IR ;
WARD, MS .
FUSION TECHNOLOGY, 1995, 27 (03) :201-214
[7]   PARAMETER SPACE FOR MAGNETIZED FUEL TARGETS IN INERTIAL CONFINEMENT FUSION [J].
LINDEMUTH, IR ;
KIRKPATRICK, RC .
NUCLEAR FUSION, 1983, 23 (03) :263-284
[8]   The fundamental parameter space of controlled thermonuclear fusion [J].
Lindemuth, Irvin R. ;
Siemon, Richard E. .
AMERICAN JOURNAL OF PHYSICS, 2009, 77 (05) :407-416
[9]   Convective instability of radiatively cooling self-similar implosions [J].
Murakami, M ;
Nishihara, K .
PHYSICS OF PLASMAS, 2000, 7 (07) :2978-2986