This article reports, for the first time, two-dimensional magnetohydrodynamic liner-on-plasma simulations for the compression phase of a magnetized target fusion (MTF) system with an inverse Z-pinch target. These simulations evolve the complete liner-plasma system along with the driving pulsed-power source. First, it has been demonstrated that closely coupled liner-on-plasma simulations produce results that are significantly different from loosely coupled simulations that have been reported in the literature. Second, it has been found that an initially stable plasma, satisfying the Kadomtsev criteria, and with a small initial pressure perturbation in the axial direction, remains stable all through the compression phase, even though there are large changes in the pressure and magnetic field levels. Third, a plasma that violates the Kadomtsev criteria, even by a small amount, turns out to be unstable, as predicted by theory. In practical terms, this means that it is preferable to stay well away from the stability limit, even at the cost of some reduction of initial plasma pressure. Fourth, even during the burn phase, when there is a large and rapid increase in plasma pressure due to fusion energy deposition, an initially stable plasma generally tends to remain stable, and even improves its stability margin. This observation shows that the inverse Z pinch is fairly benign as a MTF target, as an initially stable plasma remains stable during both the compression and burn phases. Fifth, certain unusual features are observed in the temperature profile—these depend upon the time scale for implosion. This has implications for plasma-surface interactions at the liner and central conductor.
model, based upon the Lindemann melting law, will be used later. We have performed 2D lagrangian MHD simulations for HEL and quasi-spherical liner systems in a Z-pinch configuration. For the HEL system, we have obtained II.COMPUTATIONAL DETAILS reasonable agreement with the experimental values of liner velocity, kinetic energy and the liner shape.We have performed computer simulations for two In quasi-spherical liner system simulation, there is a experimental systems, details of which are available in the good match with published results for the liner shape and literature. These are the High Energy Liner (HEL) [3] and radius until t = 12.7 gs. Also, our simulation indicates the quasi-spherical liner acceleration [4] experiments. melting, but no vaporization, as reported in the literature. Details are given in the following sub-sections.However, as convergence proceeds toward the axis, we find large distortions in the inner surface of the liner, A. High Energy Liner (HEL) system which do not allow the simulation to continue beyondThe HEL system [3] consists of a thin cylindrical shell 14.4 gs. This is a major mismatch with 2D MHD made of aluminum, having a thickness of 4 mm. It has an simulations reported in the literature.initial outer radius of 240 mm and a length of 100 mm.
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