磁压缩实验中壁面加热和杂质混合的考虑

R. Faehl, I. Lindemuth, R. Siemon, T. Awe
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引用次数: 1

摘要

本文给出了当表面磁场随时间变化时磁场在金属材料中的输运的解析处理。这在大电流脉冲功率领域有许多应用。我们在本文中重点研究其中的一种,磁化靶聚变(MTF),这是一种简单、潜在廉价的方法,通过快速压缩致密、温暖的磁化等离子体来创造燃烧聚变条件。等离子体电子的磁化,需要抑制热输运损失,这意味着压缩,在10微秒(10-5秒)的数量级,导致大磁场压缩。电流密度J与壁面的场梯度成正比,也可以用解析法得到。墙体的加热也是etaJ2的一个函数,因此也可以用这些解来评估。拟在ATLAS脉冲功率设施(23兆焦耳,30毫安,240千伏)进行的MTF研究必须明确确定壁面的能量耗散。金属壁材料的蒸发,甚至可能是熔化,可能导致这种高z材料与热氢等离子体的混合。随之而来的辐射损失和等离子体冷却对任何MTF计划都是灾难性的。
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Wall Heating and Impurity Mixing Considerations During Magnetic Compression Experiments
We present an analytic treatment of the transport of magnetic field into a metallic material, when the surface field is changing in time. This has many applications in the area of high-current pulsed power. We focus on one of these in this paper, magnetized target fusion (MTF), a simple, potentially inexpensive method of creating burning fusion conditions through fast compression of dense, warm magnetized plasma. Magnetization of the plasma electrons, needed to inhibit thermal transport losses, means that compression, on the order of 10 microseconds (10-5 seconds), results in large magnetic field compression. Current density, J, proportional to the field gradient in the walls, is also found analytically. Heating in the wall is also a function of etaJ2, and so can also be evaluated with these solutions. MTF studies proposed to be conducted at the ATLAS pulsed-power facility (23 MJ, 30 MA, 240 kV), must explicitly determine energy dissipation in the wall. Vaporization, or possibly even melting, of metallic wall material could lead to mixing of such high-Z material with the hot hydrogen plasma. The ensuing radiation losses and plasma cooling would be catastrophic to any MTF scheme.
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