MHD通道中钾原子密度分布和等离子体温度分布

Y. Aoki, H. Kitagawa, K. Sumi, S. Oikawa, N. Kayukawa, H. Yamazaki
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引用次数: 0

摘要

通过实验确定了磁流体动力学等离子体中钾原子密度N/sub k/所需的自然阻尼比a′的值。讨论了测量频率的选择。结果表明,在1700 ~ 2300 k温度范围内,当钾原子占总组分的1 wt.%时,乙醇燃烧等离子体的N/sub - k/在10/sup 22/-10/sup 23/ m/sup -3/范围内。由于在上述温度范围内,燃烧气体等离子体中的总颗粒数为3*10/sup 24/约4*10/sup 24/ m/sup -3/,因此钾原子的摩尔分数占总组分的百分比为5*10/sup -3/约3*10/sup -2/。这个值比化学反应平衡条件下得到的钾原子的摩尔分数大得多。这被认为是实验中产生水滴的主要原因,并极大地影响了固态种子材料的光学测量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The potassium atom density distribution and plasma temperature profile in an MHD channel
The value of the natural damping ratio, a', which is needed to calculate the density, N/sub k/, of potassium atoms in a magnetohydrodynamic plasma, has been determined experimentally. The choice of measurement frequency is discussed. The results showed that N/sub k/ in an ethyl-alcohol combustion plasma in which the potassium atom is 1 wt.% of the total components and at a temperature between 1700 and 2300 K is within the range 10/sup 22/-10/sup 23/ m/sup -3/. Since the total particle count in the combustion gas plasma is 3*10/sup 24/ approximately 4*10/sup 24/ m/sup -3/ in the above temperature range, the mol fraction of the potassium atoms as a percentage of the total components is 5*10/sup -3/ approximately 3*10/sup -2/. This value is much larger than the mol fraction of potassium atoms obtained under conditions of chemical reaction equilibrium. This is considered to be the chief cause of water drops during experiments and greatly influences the optical measurement of solid-state seed materials.<>
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