4.4 Article Proceedings Paper

Pulsed-power-driven high energy density physics and inertial confinement fusion research

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PHYSICS OF PLASMAS
卷 12, 期 5, 页码 -

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AIP Publishing
DOI: 10.1063/1.1891746

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The Z accelerator [R. B. Spielman, W. A. Stygar, J. F. Seamen , Proceedings of the 11th International Pulsed Power Conference, Baltimore, MD, 1997, edited by G. Cooperstein and I. Vitkovitsky (IEEE, Piscataway, NJ, 1997), Vol. 1, p. 709] at Sandia National Laboratories delivers similar to 20 MA load currents to create high magnetic fields (> 1000 T) and high pressures (megabar to gigabar). In a z-pinch configuration, the magnetic pressure (the Lorentz force) supersonically implodes a plasma created from a cylindrical wire array, which at stagnation typically generates a plasma with energy densities of about 10 MJ/cm(3) and temperatures > 1 keV at 0.1% of solid density. These plasmas produce x-ray energies approaching 2 MJ at powers > 200 TW for inertial confinement fusion (ICF) and high energy density physics (HEDP) experiments. In an alternative configuration, the large magnetic pressure directly drives isentropic compression experiments to pressures > 3 Mbar and accelerates flyer plates to > 30 km/s for equation of state (EOS) experiments at pressures up to 10 Mbar in aluminum. Development of multidimensional radiation-magnetohydrodynamic codes, coupled with more accurate material models (e.g., quantum molecular dynamics calculations with density functional theory), has produced synergy between validating the simulations and guiding the experiments. Z is now routinely used to drive ICF capsule implosions (focusing on implosion symmetry and neutron production) and to perform HEDP experiments (including radiation-driven hydrodynamic jets, EOS, phase transitions, strength of materials, and detailed behavior of z-pinch wire-array initiation and implosion). This research is performed in collaboration with many other groups from around the world. A five year project to enhance the capability and precision of Z, to be completed in 2007, will result in x-ray energies of nearly 3 MJ at x-ray powers > 300 TW. (c) 2005 American Institute of Physics.

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