电热不稳定性作为加速烧蚀箔磁-瑞利-泰勒不稳定性种子的实验

A. Steiner, D. Yager-Elorriaga, P. Campbell, S. Patel, N. Jordan, Y. Lau, R. Gilgenbach
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摘要

只提供摘要形式。当载流材料的电阻率取决于温度时,就会出现电热不稳定性(ETI)。当电阻率η随温度升高而增大时,ETI引起与电流方向垂直的条纹形成。在脉冲功率驱动的烧蚀金属载荷下,这一过程会导致目标的部分比大块材料更早地烧蚀,从而在等离子体-真空界面上产生宏观表面扰动。实验正在密歇根大学的MAIZE 1- ma线性变压器驱动器上进行,以研究ETI产生的表面扰动作为内爆衬垫[1]和加速箔等离子体[2]上瑞利-泰勒(MRT)不稳定性的种子。目标箔是在UM的Lurie纳米制造工厂通过在1.5 μm的Chemplex Ultra-Polyester薄膜上沉积超薄(200至500 nm)的铝或钛涂层来制造的。选择箔的厚度是为了保证每次射击之间的质量相同,选择的材料是为了提供明显不同的dη/dt值,这影响了电热不稳定性的增长速度。通过在MAIZE上驱动500至600 kA的电流来烧蚀和加速目标,并且使用12帧激光成像系统对加速的等离子体进行成像。这些等离子体的图像进行比较,以确定是否初始等离子体界面扰动在不同材料的目标上是可测量的不同,具有相同的质量,但不同的ETI增长率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Experiments on electrothermal instability as a seed for Magneto-Rayleigh-Taylor instability on accelerating, ablating foils
Summary form only given. The electrothermal instability (ETI) arises whenever a current-carrying material has a resistivity that depends on temperature. When resistivity, η, increases with increasing temperature, ETI causes striations to form perpendicular to the direction of current. On pulsed-power-driven, ablating metallic loads, this process can cause sections of the target to ablate earlier than the bulk material, creating a macroscopic surface perturbation on the plasma-vacuum interface. Experiments are underway on the MAIZE 1-MA linear transformer driver at the University of Michigan to study surface perturbations produced by ETI as seeding for the Rayleigh-Taylor (MRT) instability on imploding liner [1] and accelerating foil plasmas [2]. Target foils are fabricated at the Lurie Nanofabrication Facility at UM by depositing ultrathin (200 to 500 nm) coatings of aluminum or titanium on 1.5 μm Chemplex Ultra-Polyester films. Foil thicknesses are chosen to maintain the same mass between shots, and the materials are chosen to provide substantially different values of dη/dt, which impacts the growth rate of the electrothermal instability. Targets are ablated and accelerated by driving a current of 500 to 600 kA on MAIZE, and the accelerated plasmas are imaged using a 12-frame laser imaging system. Images of these plasmas are compared to determine if initial plasma interface perturbations are measurably different on targets of different materials, with the same mass, but different ETI growth rates.
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