Magnetic Diagnostics of Magnetic Island in LHD
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- NARUSHIMA Y.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- WATANABE K. Y.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- SAKAKIBARA S.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- OHYABU N.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- YAMADA H.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- NARIHARA K.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- YAMADA I.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- MORISAKI T.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- INAGAKI S.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- NAGAYAMA Y.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- KOMORI A.
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- LHD exp. group
- National Institute for Fusion Science, Toki, Gifu 509-5292, Japan
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- COOPER W. A.
- CRPP Association Euratom / Confederartion Suisse, EPFL, 1015 Lausanne, Switzerland
説明
Characteristics of magnetic islands are investigated by magnetic diagnostics in the Large Helical Device (LHD). The structure of the magnetic island with m/n = 1/1 (where, m and n are poloidal and toroidal mode number, respectively) can be estimated from the perturbed magnetic field appearing when a magnetic island changes. To measure the toroidal profile of the perturbed magnetic field δb1 originating from the plasma, a toroidal array of magnetic flux loops is set up in the LHD. The toroidal profile of δb1 is then spatially Fourier decomposed to determine the amplitude of the n = 1 component, δb1n=1 and its phase, φn=1 which correspond the change of the island width and the toroidal position of the X-point of the island, respectively. Therefore, the information about the magnetic island structure can be obtained from δb1n=1 and φn=1. In case the island width becomes larger than the seed island, measurements show that δb1n=1 is non-zero and φn=1 is temporally constant. A non-zero δb1n=1 can also be observed when the island width becomes smaller than the seed island. In this case, the angle φn=1 shifts by about π[rad] compared with the increasing case and the δb1n=1 is limited to a certain value which corresponding to the magnetic field suppressing the seed island.
収録刊行物
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- Plasma and Fusion Research
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Plasma and Fusion Research 2 S1094-S1094, 2007
一般社団法人 プラズマ・核融合学会
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詳細情報 詳細情報について
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- CRID
- 1390001205255413888
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- NII論文ID
- 120005964085
- 130002058983
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- ISSN
- 18806821
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- HANDLE
- 10655/6394
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- 本文言語コード
- en
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- データソース種別
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- JaLC
- IRDB
- Crossref
- CiNii Articles
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- 抄録ライセンスフラグ
- 使用不可