磁约束热核聚变反应堆的能量约束时间

C. Chen, J. Becker, J. J. Farrell
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引用次数: 0

摘要

聚变研究中最重要的一个科学问题可能是聚变等离子体中的约束[1]。本文综述了最近发展的一种理论模型[2],用于描述发生聚变反应的材料中离子动能的约束时间。在理论模型中,离子停止被认为是离子动能损失的关键机制,得到了D-T等离子体中离子动能约束时间的估计,发现比劳森准则要求的要低几个数量级。自发电子回旋辐射被认为是磁约束等离子体中电子动能损失的重要机制,因为离子通过离子停止将其动能传递给电子,离子与电子之间发生热化。得到的能量约束时间与TFTR[1]和Wendelstein 7-X[3]的测量结果一致。得到了一个适用于磁约束热核聚变反应堆的先进的劳森判据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Energy Confinement Time in a Magnetically Confined Thermonuclear Fusion Reactor
The single most important scientific question in fusion research may be confinement in a fusion plasma [1] . A recently-developed theoretical model [2] is reviewed for the confinement time of ion kinetic energy in a material where fusion reactions occur. In the theoretical model where ion stopping was considered as a key mechanism for ion kinetic energy loss, an estimate was obtained for the confinement time of ion kinetic energy in a D-T plasma - and found to be orders of magnitude lower than required in the Lawson criterion. As ions transfer their kinetic energies to electrons via ion stopping and thermalization between the ions and the electrons takes place, spontaneous electron cyclotron radiation is identified as a key mechanism for electron kinetic energy loss in a magnetically confined plasma. The energy confinement time is obtained and found in agreement with measurements from TFTR [1] and Wendelstein 7-X [3] . An advanced Lawson criterion is obtained for a magnetically confined thermonuclear fusion reactor.
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