摘要
根据MHD气球模稳定性理论,计算了负磁剪切位形中等离子体气球边缘稳定性区域。结果表明,在同样参数下,负磁剪切区域比正磁剪切区域允许更大的β值。
Based on MHD ballooning mode stability theory, marginal stability regions of the plasma ballooning mode in negative magnetic shear configuration are calculated in this paper. The results show that the negative magnetic shear region permits larger β value than positive region under the same parameters.
出处
《核聚变与等离子体物理》
CAS
CSCD
北大核心
1998年第4期21-24,共4页
Nuclear Fusion and Plasma Physics
基金
国家自然科学基金