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Radiative losses and improvement of plasma parameters after gettering in the Advanced Toroidal Facility

R.C. Isler, E.C. Crume, L.D. Horton, M. Murakami, L.R. Baylor, G.L. Bell, T.S. Bigelow, A.C. England, J.C. Glowienka, T.C. Jernigan1991年被引用 15Nuclear FusionIF 3出版社

The characteristics of plasmas in the Advanced Toroidal Facility (ATF) have proven to be strongly dependent on the type of wall conditioning employed. A succession of techniques, beginning with glow discharge cleaning and baking, and evolving to gettering with chromium and titanium, have led to progressive improvement of the plasma parameters. Gettering with titanium has reduced the low-Z impurity content by a factor of 3, lowered the radiated power by a factor of 2.5–3.5, and improved the control over the electron density. The maximum values achieved for stored energy, line averaged density and confinement times are 28 kJ, 1.2 × 1014cm−3 and 25 ms, respectively. These parameters are comparable to the best results achieved in the ISX-B tokamak which had the same average minor radius and one half the major radius of ATF. Quasi-steady operation for 200 ms of neutral beam injection (NBI) has been obtained in high density, titanium gettered plasmas without the collapses that were typical earlier periods of operation. Neon injection experiments have helped to delineate the limits on the global levels of radiation that can be maintained and have supported the conclusion that mechanisms other than radiative losses are important for initiating the collapses still observed in low density NBI plasmas.

日本語訳

Advanced Toroidal Facility (ATF)におけるプラズマの特性は、使用する壁調整の種類に強く依存することが実証された。グロー放電洗浄とベーキングから始まり、クロムおよびチタンによるゲッタリングへと発展してきた一連の技術により、プラズマパラメータは段階的に改善された。チタンによるゲッタリングにより、低Z不純物含有量は3分の1に低減され、放射パワーは2.5〜3.5倍低減され、電子密度の制御が改善された。蓄積エネルギー、線平均密度、閉じ込め時間の最大値は、それぞれ28 kJ、1.2×10¹⁴cm⁻³、25 msに達した。これらのパラメータは、ATFと同じ平均小半径とその半分の大半径を有するISX-Bトカマクで達成された最高の結果に匹敵する。高密度のチタンゲッタリングプラズマにおいて、200ミリ秒の準定常運転が、初期の運転期間に典型的に見られた崩壊を伴わずに達成された。ネオン入射実験は、維持可能な全体的な放射レベルの限界を明らかにするのに役立ち、低密度NBIプラズマで依然として観測される崩壊を開始するには、放射損失以外のメカニズムが重要であるという結論を裏付けるものである。

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