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Dipole moment of the Pfirsch-Schluter current in a finite beta stellarator plasma in Heliotron E

S. Besshou, N. Fujita, K. Ogata, K. Kondo, Y. Kurimoto, T. Mizuuchi, K. Nagasaki, H. Okada, F. Sano, T. Obiki1997年被引用 7Nuclear FusionIF 3出版社

A magnetic determination of the dipole moment of the Pfirsch-Schluter current in a finite beta stellarator/heliotron plasma is described. The rotating cosine saddle diagnostic coils and the poloidal flux loops are used to identify the dipole current in a finite beta toroidal plasma. A typical dipole moment of the toroidal current in the standard Heliotron E configuration is 0.6 kA m, when the volume averaged beta is 0.50% at a magnetic field of 0.94 T. The measured equilibrium dipole current is practically proportional to the diamagnetic volume average beta available up to 0.95%. The observed dipole moment of the Pfirsch-Schluter current is compared with a magnetohydrodynamic (MHD) calculation for a finite beta stellarator plasma

日本語訳

有限ベータ星型/ヘリオトロンプラズマにおけるプフィルシュ・シュリューター電流の双極子モーメントの磁気的決定について述べる。回転コサインサドル診断コイルとポロイダル磁束ループを用いて、有限ベータトロイダルプラズマ中の双極子電流を同定する。標準的なヘリオトロンE配位におけるトロイダル電流の典型的な双極子モーメントは、磁場0.94 Tにおいて体積平均ベータが0.50%のとき、0.6 kA mである。測定された平衡双極子電流は、利用可能な0.95%までの反磁性体積平均ベータに実質的に比例する。観測されたプフィルシュ・シュリューター電流の双極子モーメントは、有限ベータ星型プラズマに対する磁気流体力学(MHD)計算と比較される。

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