Published June 2007 | Version v1
Journal article

One- and two-dimensional modeling of argon K-shell emission from gas-puff Z-pinch plasmas

  • 1. National Nuclear Security Administration, Washington, D.C. 20585 (United States)
  • 2. Sandia National Laboratories, Albuquerque, New Mexico 87185 (United States)
  • 3. Alameda Applied Sciences, San Leandro, California 94577 (United States)
  • 4. L-3 Communications/Pulse Sciences, San Leandro, California 94577 (United States)
  • 5. NumerEx, Albuquerque, New Mexico 87106 (United States)
  • 6. Berkeley Scholars, Beltsville, Maryland 20705 (United States)
  • 7. Plasma Physics Division, Naval Research Laboratory, Washington, D.C. 20375 (United States)

Description

In this paper, a theoretical model is described and demonstrated that serves as a useful tool for understanding K-shell radiating Z-pinch plasma behavior. Such understanding requires a self-consistent solution to the complete nonlocal thermodynamic equilibrium kinetics and radiation transport in order to realistically model opacity effects and the high-temperature state of the plasma. For this purpose, we have incorporated into the MACH2 two-dimensional magnetohydrodynamic (MHD) code [R. E. Peterkin et al., J. Comput. Phys. 140, 148 (1998)] an equation of state, called the tabular collisional radiative equilibrium (TCRE) model [J. W. Thornhill et al., Phys. Plasmas 8, 3480 (2001)], that provides reasonable approximations to the plasma's opacity state. MACH2 with TCRE is applied toward analyzing the multidimensional implosion behavior that occurred in Decade Quad (DQ) [D. Price et al., Proceedings of the 12th IEEE Pulsed Power Conference, Monterey, CA, edited by C. Stallings and H. Kirbie (IEEE, New York, 1999), p. 489] argon gas puff experiments that employed a 12 cm diameter nozzle with and without a central gas jet on axis. Typical peak drive currents and implosion times in these experiments were ∼6 MA and ∼230 ns. By using Planar Laser Induced Fluorescence measured initial density profiles as input to the calculations, the effect these profiles have on the ability of the pinch to efficiently produce K-shell emission can be analyzed with this combined radiation-MHD model. The calculated results are in agreement with the experimental result that the DQ central-jet configuration is superior to the no-central-jet experiment in terms of producing more K-shell emission. These theoretical results support the contention that the improved operation of the central-jet nozzle is due to the better suppression of instabilities and the higher-density K-shell radiating conditions that the central-jet configuration promotes. When we applied the model toward projecting argon K-shell yield behavior for Sandia National Laboratories' ZR machine (∼25 MA peak drive currents, ∼100 ns implosion times) [D. McDaniel et al., Proceedings of the 5th International Conference on Dense Z-Pinches, Albuquerque, NM, 2002, edited by J. Davis, C. Deeney, and N. R. Pereira (American Institute of Physics, New York, 2002), Vol. 651, p. 23] for experiments that utilize the 12 cm diameter central-jet nozzle configuration, it predicts over 1 MJ of K-shell emission is attainable

Additional details

Identifiers

Publishing Information

Journal Title
Physics of Plasmas
Journal Volume
14
Journal Issue
6
Journal Page Range
p. 063301-063301.14
ISSN
1070-664X
CODEN
PHPAEN

Optional Information

Notes
(c) 2007 American Institute of Physics