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Observations on the W-transport in the core plasma of JET and ASDEX Upgrade

T Pütterich, R Dux, R Neu, M Bernert, M N A Beurskens, V Bobkov, S Brezinsek, C Challis, J W Coenen, I Coffey2013年Plasma Physics and Controlled FusionIF 2.2出版社

The W-transport in the core plasma of JET is investigated experimentally by deriving the W-concentration profiles from the modelling of the signals of the soft x-ray cameras. For the case of pure neutral beam heating W accumulates in the core (r/a < 0.3) approaching W-concentrations of 10−3 in between the sawtooth crashes, which flatten the W-profile to a concentration of about 3 × 10−5. When central Ion cyclotron resonant heating is additionally applied the core W-concentration decays in phases that exhibit a changed mode activity, while also the electron temperature increases and the density profile becomes less peaked. The immediate correlation between the change of magnetohydrodymanic (MHD) and the removal of W from the plasma core supports the hypothesis that the change of the MHD activity is the underlying cause for the change of transport. Furthermore, a discharge from the ASDEX Upgrade is investigated. In this case the plasma profiles exhibit small changes only, while the most prominent change occurs in the W-content of the confined plasma caused by the reduction of the fuelling deuterium gas puff. Concomintantly, the W-concentration profiles in the core plasma r/a < 0.2 steepen up reminescent to the well-known connection between central radiation and transport during cases with strong, established W-accumulation, while in the present analysis such a causality between the two during the onset of W-accumulation could not be pinned down. Both case studies exemplify that small changes of the core parameters of a plasma my influence the W-transport in the plasma core drastically.

日本語訳

JETのコアプラズマにおけるW輸送は、軟X線カメラの信号のモデリングからW濃度分布を導出することにより実験的に調査される。純粋な中性粒子ビーム加熱の場合、Wはコア部(r/a < 0.3)に蓄積し、鋸歯状振動の間にW濃度は10⁻³に近づくが、鋸歯状振動はW分布を約3×10⁻⁵の濃度まで平坦化する。中心イオンサイクロトロン共鳴加熱を追加で適用すると、コアW濃度は、モード活動の変化を示す位相において減衰する一方、電子温度は上昇し、密度分布はより平坦でなくなる。MHD活動の変化とプラズマコアからのWの除去との間の即時的な相関は、MHD活動の変化が輸送の変化の根本的な原因であるという仮説を支持する。さらに、ASDEX Upgradeからの放電が調査される。この場合、プラズマ分布はわずかな変化のみを示す一方、最も顕著な変化は、重水素ガスパフの低減による閉じ込めプラズマのW含有量に生じる。同時に、コアプラズマ(r/a < 0.2)におけるW濃度分布は急峻化し、これは、強いW蓄積が確立された期間中の中心放射と輸送との間のよく知られた関係を想起させる。しかしながら、本解析では、W蓄積の開始期間中における両者の間の因果関係は特定できなかった。両方のケーススタディは、プラズマコアのパラメータの小さな変化が、コアプラズマにおけるW輸送に劇的な影響を与え得ることを例証している。

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