在extra‐T1反场夹紧实验中研究了高杂质回收时的总辐射功率损耗和部分辐射功率损耗

K. Zastrow, J. Brzozowski
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引用次数: 6

摘要

辐射功率损耗的测量是在Extrap - T1反向场捏缩上进行的。Scr. 44, 358(1991)]使用绝对校准的真空紫外光谱仪,波长范围在100和1700 A之间。测量了氘、碳、氮、氧和氯对辐射功率损失的贡献。这些部分辐射功率损失进一步划分为这些杂质的不同电离阶段的贡献。估计了电离过程对冷却速率的额外贡献。发现杂质是放电初期功率损失的主要原因。在放电结束时,由于电子密度的降低,辐射功率损失小于输入功率的10%。由于粒子约束时间短,杂质(特别是氧)的再循环率高,每离子辐射功率损失的速率系数仅随温度的增加而略有降低。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Total and partial radiative power loss at high impurity recycling studied in the Extrap‐T1 reversed‐field pinch experiment
Measurements of the radiative power loss are performed on the Extrap‐T1 reversed‐field pinch [Phys. Scr. 44, 358 (1991)] using an absolutely calibrated vacuum ultraviolet spectrometer in the wavelength range between 100 and 1700 A. The contributions to the radiative power loss from deuterium, carbon, nitrogen, oxygen, and chlorine are measured. These partial radiative power losses are further divided into contributions from different ionization stages of these impurities. The additional contribution to the cooling rate due to ionization processes is estimated. Impurities are found to be a main contributor to the power loss in the initial phase of the discharge. Toward the end of the discharge, radiative power loss amounts to less than 10% of the input power, due to the decrease of the electron density. Because of the short particle confinement time and high recycling of impurities, specifically oxygen, the rate coefficient for radiative power loss per ion is only slightly reduced by the increase of the te...
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