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Molybdenum test limiter experiments in TEXTOR

V. Philipps, T. Tanabe, Y. Ueda, A. Pospieszczyk, M.Z. Tokar, B. Unterberg, L. Konen, B. Schweer, U. Samm, P. Wienhold1994年被引用 68Nuclear FusionIF 3出版社

Limiter experiments with a Mo test limiter have been carried out in TEXTOR under various conditions with ohmic and NBI heating. Maximum power loads reached about 20 MW/m2 resulting in surface temperatures up to the melting point. A maximum fraction of 8% of the total convective energy in the plasma was deposited onto the Mo limiter. Molybdenum impurities are mainly produced by physical sputtering due to the impact of C and O impurities. Under ohmic heating conditions the Mo impurity radiation increased with increasing plasma density, though the relative source strength of the Mo release decreased. Approaching a critical density of about 3*1013 cm-3 Mo accumulated in the plasma centre leading to strong central radiation with hollow temperature profiles, which resulted in a minor disruption. Under NBI heated plasma conditions (co-NBI, 1.3 MW) Mo radiation decreased with increasing plasma density as did the relative Mo source at the limiter; at high plasma densities the influence of the Mo limiter on plasma impurities and plasma performance became negligible. No instability was observed under these conditions. The different behaviour between ohmic and NBI heating conditions is explained by the different relative importance of neoclassical and anomalous transport under ohmic and NBI heating, respectively. The observed instability in high density ohmic plasmas is caused by Mo accumulation in the plasma centre and is attributed to neoclassical transport processes

日本語訳

リミッターを用いた実験は、様々な条件下でTEXTORにおいてオーミック加熱およびNBI加熱により実施された。最大出力負荷は約20 MW/m²に達し、表面温度は融点にまで達した。プラズマ中の全対流エネルギーの最大8%がMoリミッターに堆積した。モリブデン不純物は主に、CおよびO不純物の衝突による物理スパッタリングによって生成された。オーミック加熱条件下では、Mo不純物放射はプラズマ密度の増加とともに増加したが、Mo放出の相対的な源強度は減少した。臨界密度約3×10¹³ cm⁻³に近づくと、Moがプラズマ中心部に蓄積し、中心部の温度分布が平坦化する強い放射が生じ、その結果、小さなディスラプションが発生した。NBI加熱条件下(コNBI、1.3 MW)では、Mo放射はプラズマ密度の増加とともに減少し、リミッターでの相対的なMo源強度も同様に減少した。高密度時には、Moリミッターがプラズマ不純物およびプラズマ性能に及ぼす影響は無視できるほどになった。これらの条件下では不安定性は観測されなかった。オーミック加熱とNBI加熱の間の挙動の違いは、それぞれの加熱条件下での新古典輸送と異常輸送の相対的な重要性の違いによって説明される。高密度オーミックプラズマで観測された不安定性は、Moの中心部への蓄積によって引き起こされ、新古典輸送過程に起因するものである。

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