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The Challenge of Wall-Plasma Interaction with Pulsed Megagauss Magnetic Fields

机译:脉冲等离子体高斯磁场与壁等离子体相互作用的挑战

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A method is described for choosing experimental parameters in studies of high-energy-density (HED) physics relevant to fusion energy, as well as other applications. An important HED issue for magneto-inertial fusion (MIF) is the interaction of metal pusher materials with megagauss (MG) magnetic fields during liner compression of magnetic flux and fusion fuel. The experimental approach described here is to study a stationary conductor when a pulsed current generates MG fields at the surface, instead of studying the inner surface of a moving liner. This places less demand upon the pulsed power system, and significantly improves diagnostic access. Thus the deceptively simple geometry chosen for this work is that of a z pinch composed of a metal cylinder carrying large current. Consideration of well known stability issues for the z pinch shows that for given peak current and rise time from a particular power supply, there is a minimum radius and thus maximum B field that can be created without disruption of the conductor before peak current. The reasons are reviewed why MG levels of magnetic field, as required for MIF, result in high temperatures and plasma formation at the surface of the metal in response to Ohmic heating. The distinction is noted between the liner regime obtained with cylindrical rods, which have a skin depth small compared to the conductor radius, and the exploding thin-wire regime, which has skin depth larger than the wire radius. A means of diagnostic development is described using a small facility (DPM15) built at the University of Nevada, Reno. It is argued that surface plasma temperature measurements in the 10-eV range are feasible based on the intensity of visible light emission.
机译:描述了一种在与聚变能有关的高能密度(HED)物理研究以及其他应用中选择实验参数的方法。磁惯性聚变(MIF)的一个重要的HED问题是在磁通量和聚变燃料的衬里压缩过程中,金属推动材料与高斯(MG)磁场的相互作用。这里描述的实验方法是研究脉冲电流在表面上产生MG场时的固定导体,而不是研究活动衬套的内表面。这减少了对脉冲电源系统的需求,并显着提高了诊断能力。因此,为这项工作选择的看似简单的几何形状是z夹点的形状,该夹点由承载大电流的金属圆柱体组成。对z夹点的众所周知的稳定性问题的考虑表明,对于给定的峰值电流和来自特定电源的上升时间,存在一个最小半径,因此可以产生最大B场,而不会在峰值电流之前中断导体。综述了为什么MIF所需的MG磁场强度会导致金属在高温下响应欧姆加热而在金属表面形成等离子体的原因。注意到在用圆柱形杆获得的衬里状态(其趋肤深度比导体半径小)和爆炸的细线状态(其趋肤深度大于导线半径)之间的区别。使用内华达大学里诺分校的小型设备(DPM15)描述了一种诊断开发方法。有人认为,基于可见光的发射强度,在10 eV范围内进行表面等离子体温度测量是可行的。

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