Current channel evolution in ideal Z pinch for general velocity profiles

Recent diagnostic advances in gas-puff Z pinches at the Weizmann Institute for the first time allow the reconstruction of the current flow as a function of time and radius. These experiments show an unexpected radially-outward motion of the current channel, as the plasma moves radially-inward [C. Stollberg, Ph.D thesis, Weizmann Institute, 2019]. In this paper, a mechanism that could explain this current evolution is described. We examine the impact of advection on the distribution of current in a cylindrically symmetric plasma. In the case of metric compression, with |v_r| proportional to r, the current enclosed between each plasma fluid element and the axis is conserved, and so the current profile maintains its shape. We show that for more general velocity profiles, this simple behavior quickly breaks down, allowing for non-conservation of current in a compressing conductor, rapid redistribution of the current density, and even for the formation of reverse currents. In particular, a specific inward radial velocity profile is shown to result in radially-outward motion of the current channel, recovering the surprising current evolution discovered at the Weizmann Institute.

[1]  G. Rosenzweig,et al.  Measurements of the spatial magnetic field distribution in a z-pinch plasma throughout the stagnation process , 2017 .

[2]  J. Giuliani,et al.  A Review of the Gas-Puff $Z$ -Pinch as an X-Ray and Neutron Source , 2015, IEEE Transactions on Plasma Science.

[3]  D. Hammer,et al.  Determination of magnetic fields based on the Zeeman effect in regimes inaccessible by Zeeman-splitting spectroscopy , 2014 .

[4]  A. Velikovich,et al.  Effective versus ion thermal temperatures in the Weizmann Ne Z-pinch: Modeling and stagnation physics , 2014 .

[5]  C. Jennings,et al.  Pressure and energy balance of stagnating plasmas in z-pinch experiments: implications to current flow at stagnation. , 2013, Physical review letters.

[6]  M. Cuneo,et al.  Ion temperature and hydrodynamic-energy measurements in a Z-pinch plasma at stagnation. , 2011, Physical review letters.

[7]  J. Giuliani,et al.  Evolution of MHD Instabilities in Plasma Imploding Under Magnetic Field , 2011, IEEE Transactions on Plasma Science.

[8]  M. Haines,et al.  A review of the dense Z-pinch , 2011 .

[9]  U. Shumlak,et al.  Note: Zeeman splitting measurements in a high-temperature plasma. , 2010, The Review of scientific instruments.

[10]  A. Lichtenberg,et al.  Principles of Plasma Discharges and Materials Processing: Lieberman/Plasma 2e , 2005 .

[11]  U. Shumlak,et al.  Formation of a sheared flow Z pinch , 2005 .

[12]  Lee,et al.  Reversed current structure in a Z-pinch plasma , 2000, Physical review letters.

[13]  Y. Maron,et al.  Spectroscopic determination of the magnetic-field distribution in an imploding plasma , 1998 .

[14]  Fisher,et al.  Particle velocity distributions and ionization processes in a gas-puff Z pinch. , 1994, Physical review letters.

[15]  A. Fruchtman Penetration and expulsion of magnetic fields in plasmas due to the Hall field , 1991 .

[16]  G. Rickard,et al.  The nature of the inverse skin effect , 1989 .

[17]  R. Kulsrud,et al.  Analysis of anomalous resistivity during the conduction phase of the plasma erosion opening switch: Interim report , 1988 .

[18]  M. Haines The Inverse Skin Effect , 1959 .

[19]  Arrow,et al.  The Physics of Fluids , 1958, Nature.