Solid liner implosions on Z for producing multi-megabar, shockless compressionsa)

Current pulse shaping techniques, originally developed for planar dynamic material experiments on the Z-machine [M. K. Matzen et al., Phys. Plasmas 12, 055503 (2005)], are adapted to the design of controlled cylindrical liner implosions. By driving these targets with a current pulse shape that prevents shock formation inside the liner, shock heating is avoided along with the corresponding decrease in electrical conductivity ahead of the magnetic diffusion wave penetrating the liner. This results in an imploding liner with a significant amount of its mass in the solid phase and at multi-megabar pressures. Pressures in the solid region of a shaped pulse driven beryllium liner fielded on the Z-machine are inferred to 5.5 Mbar, while simulations suggest implosion velocities greater than 50kms-1. These solid liner experiments are diagnosed with multi-frame monochromatic x-ray backlighting which is used to infer the material density and pressure. This work has led to a new platform on the Z-machine that can be used to perform off-Hugoniot measurements at higher pressures than are accessible through magnetically driven planar geometries.Current pulse shaping techniques, originally developed for planar dynamic material experiments on the Z-machine [M. K. Matzen et al., Phys. Plasmas 12, 055503 (2005)], are adapted to the design of controlled cylindrical liner implosions. By driving these targets with a current pulse shape that prevents shock formation inside the liner, shock heating is avoided along with the corresponding decrease in electrical conductivity ahead of the magnetic diffusion wave penetrating the liner. This results in an imploding liner with a significant amount of its mass in the solid phase and at multi-megabar pressures. Pressures in the solid region of a shaped pulse driven beryllium liner fielded on the Z-machine are inferred to 5.5 Mbar, while simulations suggest implosion velocities greater than 50kms-1. These solid liner experiments are diagnosed with multi-frame monochromatic x-ray backlighting which is used to infer the material density and pressure. This work has led to a new platform on the Z-machine that can be ...

[1]  G. R. Bennett,et al.  Measurements of magneto-Rayleigh–Taylor instability growth during the implosion of initially solid metal liners a) , 2011 .

[2]  W. Nellis,et al.  Equation of state of beryllium at shock pressures of 0.4–1.1 TPa (4–11 Mbar) , 1997 .

[3]  William A. Stygar,et al.  Experimental configuration for isentropic compression of solids using pulsed magnetic loading , 2001 .

[4]  M. Desjarlais,et al.  Supporting Online Material Materials and Methods Som Text Figs. S1 to S15 Table S1 References Shock-wave Exploration of the High-pressure Phases of Carbon , 2022 .

[5]  R.J. Faehl,et al.  Results of a 100-megaampere liner implosion experiment , 2004, IEEE Transactions on Plasma Science.

[6]  Analysis of cylindrical ramp compression experiment with radiography based surface fitting method , 2012 .

[7]  R. G. Adams,et al.  Pulsed-power-driven high energy density physics and inertial confinement fusion research , 2004 .

[8]  L. P. Mix,et al.  Differential-outputB-dot andD-dot monitors for current and voltage measurements on a 20-MA, 3-MV pulsed-power accelerator , 2008 .

[9]  M. Knudson,et al.  Magnetically driven isentropic compression experiments on the Z accelerator , 2001 .

[10]  J.-P. Davis,et al.  Magnetically accelerated, ultrahigh velocity flyer plates for shock wave experiments , 2005 .

[11]  Determination of pressure and density of shocklessly compressed beryllium from x-ray radiography of a magnetically driven cylindrical liner implosion , 2011 .

[12]  S. D. Rothman,et al.  Characteristics analysis of Isentropic Compression Experiments (ICE) , 2006 .

[13]  G. R. Bennett,et al.  Monochromatic x-ray imaging experiments on the Sandia National Laboratories Z facility (invited) , 2004 .

[14]  D. Bliss,et al.  Magnetically driven isentropic compression to multimegabar pressures using shaped current pulses on the Z accelerator , 2004 .

[15]  Gilbert W. Collins,et al.  Stiff response of aluminum under ultrafast shockless compression to 110 GPA. , 2007, Physical review letters.

[16]  M. Desjarlais Practical Improvements to the Lee‐More Conductivity Near the Metal‐Insulator Transition , 1999 .

[17]  J.-P. Davis,et al.  Magnetically driven hyper-velocity launch capability at the Sandia Z accelerator , 2011 .

[18]  Allen C. Robinson,et al.  Three-dimensional z-pinch wire array modeling with ALEGRA-HEDP , 2003, Comput. Phys. Commun..

[19]  L. J. Tabaka,et al.  Design, fabrication, and operation of a high-energy liner implosion experiment at 16 megamperes , 2002 .

[20]  C. Dasch,et al.  One-dimensional tomography: a comparison of Abel, onion-peeling, and filtered backprojection methods. , 1992, Applied optics.

[21]  M. Knudson,et al.  Equation of state measurements in liquid deuterium to 70 GPa. , 2001, Physical review letters.