Study of Plasma Current Decay in the Initial Phase of High Poloidal Beta Disruptions in JT-60U
In order to validate some current decay models during the current quench, the plasma current decay time was studied using the experimental plasma resistance and inductance in high poloidal beta, βp, disruptions in JT-60U. The plasma resistance and inductance were evaluated from an equilibrium calcul...
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Veröffentlicht in: | Plasma and Fusion Research 2011/10/21, Vol.6, pp.1302136-1302136 |
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creator | SHIBATA, Yoshihide WATANABE, Kiyomasa OHNO, Noriyasu OKAMOTO, Masaaki ISAYAMA, Akihiko KURIHARA, Kenichi OYAMA, Naoyuki NAKANO, Tomohide KAWANO, Yasunori MATSUNAGA, Go KAMADA, Yutaka SUGIHARA, Masayoshi |
description | In order to validate some current decay models during the current quench, the plasma current decay time was studied using the experimental plasma resistance and inductance in high poloidal beta, βp, disruptions in JT-60U. The plasma resistance and inductance were evaluated from an equilibrium calculation code and the measurement value of a magnetic sensor, the electron temperature evaluated by using ECE measurement and the electron density measured by FIR interferometer. In high βp disruptions, it was found that the electron temperature at the plasma center just after current quench starts was approximately 1-4 keV under almost the same current decay time observed during the initial phase of current quench. This result indicates that the electron temperature itself plays no major role in the determination of the current decay time in the initial phase of current quench. Moreover, the current decay time predicted by a modified L/R model [Y. Shibata et al., Nucl. Fusion 50, 025015 (2010)], in which the time derivative of plasma inductance was considered, was in good agreement with the experimental current decay time, while the values obtained from the conventional L/R model were two orders of magnitude larger than the experimental results. |
doi_str_mv | 10.1585/pfr.6.1302136 |
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The plasma resistance and inductance were evaluated from an equilibrium calculation code and the measurement value of a magnetic sensor, the electron temperature evaluated by using ECE measurement and the electron density measured by FIR interferometer. In high βp disruptions, it was found that the electron temperature at the plasma center just after current quench starts was approximately 1-4 keV under almost the same current decay time observed during the initial phase of current quench. This result indicates that the electron temperature itself plays no major role in the determination of the current decay time in the initial phase of current quench. Moreover, the current decay time predicted by a modified L/R model [Y. Shibata et al., Nucl. Fusion 50, 025015 (2010)], in which the time derivative of plasma inductance was considered, was in good agreement with the experimental current decay time, while the values obtained from the conventional L/R model were two orders of magnitude larger than the experimental results.</description><identifier>ISSN: 1880-6821</identifier><identifier>EISSN: 1880-6821</identifier><identifier>DOI: 10.1585/pfr.6.1302136</identifier><language>eng</language><publisher>The Japan Society of Plasma Science and Nuclear Fusion Research</publisher><subject>current decay model ; disruption ; high βp plasma discharge ; plasma inductance ; poloidal beta</subject><ispartof>Plasma and Fusion Research, 2011/10/21, Vol.6, pp.1302136-1302136</ispartof><rights>2011 by The Japan Society of Plasma Science and Nuclear Fusion Research</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4166-e0af188f094c195efd052d066e72cb40bf3ec66b714d5a7e08a0d91c2012332c3</citedby><cites>FETCH-LOGICAL-c4166-e0af188f094c195efd052d066e72cb40bf3ec66b714d5a7e08a0d91c2012332c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,1881,4022,27922,27923,27924</link.rule.ids></links><search><creatorcontrib>SHIBATA, Yoshihide</creatorcontrib><creatorcontrib>WATANABE, Kiyomasa</creatorcontrib><creatorcontrib>OHNO, Noriyasu</creatorcontrib><creatorcontrib>OKAMOTO, Masaaki</creatorcontrib><creatorcontrib>ISAYAMA, Akihiko</creatorcontrib><creatorcontrib>KURIHARA, Kenichi</creatorcontrib><creatorcontrib>OYAMA, Naoyuki</creatorcontrib><creatorcontrib>NAKANO, Tomohide</creatorcontrib><creatorcontrib>KAWANO, Yasunori</creatorcontrib><creatorcontrib>MATSUNAGA, Go</creatorcontrib><creatorcontrib>KAMADA, Yutaka</creatorcontrib><creatorcontrib>SUGIHARA, Masayoshi</creatorcontrib><title>Study of Plasma Current Decay in the Initial Phase of High Poloidal Beta Disruptions in JT-60U</title><title>Plasma and Fusion Research</title><addtitle>Plasma and Fusion Research</addtitle><description>In order to validate some current decay models during the current quench, the plasma current decay time was studied using the experimental plasma resistance and inductance in high poloidal beta, βp, disruptions in JT-60U. The plasma resistance and inductance were evaluated from an equilibrium calculation code and the measurement value of a magnetic sensor, the electron temperature evaluated by using ECE measurement and the electron density measured by FIR interferometer. In high βp disruptions, it was found that the electron temperature at the plasma center just after current quench starts was approximately 1-4 keV under almost the same current decay time observed during the initial phase of current quench. This result indicates that the electron temperature itself plays no major role in the determination of the current decay time in the initial phase of current quench. Moreover, the current decay time predicted by a modified L/R model [Y. Shibata et al., Nucl. Fusion 50, 025015 (2010)], in which the time derivative of plasma inductance was considered, was in good agreement with the experimental current decay time, while the values obtained from the conventional L/R model were two orders of magnitude larger than the experimental results.</description><subject>current decay model</subject><subject>disruption</subject><subject>high βp plasma discharge</subject><subject>plasma inductance</subject><subject>poloidal beta</subject><issn>1880-6821</issn><issn>1880-6821</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNpNkEFvwjAMhaNpk8bYjrvnD5Q5SRvaI4NtMCENaXBdFVKHBpUWJeHAv187KrSDZcv-3pP1CHlmMGJJmrwcjRvJERPAmZA3ZMDSFCKZcnb7b74nD97vAWSWMDkgP9_hVJxpY-iqUv6g6PTkHNaBzlCrM7U1DSXSRW2DVRVdlcpjB8_trqSrpmps0a5fMSg6s96djsE2te9kn-tIwuaR3BlVeXzq-5Bs3t_W03m0_PpYTCfLSMdMyghBmfZDA1msWZagKSDhBUiJY663MWyNQC3ldsziIlFjhFRBkTHNgXEhuBZDEl18tWu8d2jyo7MH5c45g7wLJ2_DyWXeh9Pykwu_90Ht8EorF6yusKfhr3rN9aZL5XKsxS-1XW4E</recordid><startdate>2011</startdate><enddate>2011</enddate><creator>SHIBATA, Yoshihide</creator><creator>WATANABE, Kiyomasa</creator><creator>OHNO, Noriyasu</creator><creator>OKAMOTO, Masaaki</creator><creator>ISAYAMA, Akihiko</creator><creator>KURIHARA, Kenichi</creator><creator>OYAMA, Naoyuki</creator><creator>NAKANO, Tomohide</creator><creator>KAWANO, Yasunori</creator><creator>MATSUNAGA, Go</creator><creator>KAMADA, Yutaka</creator><creator>SUGIHARA, Masayoshi</creator><general>The Japan Society of Plasma Science and Nuclear Fusion Research</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>2011</creationdate><title>Study of Plasma Current Decay in the Initial Phase of High Poloidal Beta Disruptions in JT-60U</title><author>SHIBATA, Yoshihide ; WATANABE, Kiyomasa ; OHNO, Noriyasu ; OKAMOTO, Masaaki ; ISAYAMA, Akihiko ; KURIHARA, Kenichi ; OYAMA, Naoyuki ; NAKANO, Tomohide ; KAWANO, Yasunori ; MATSUNAGA, Go ; KAMADA, Yutaka ; SUGIHARA, Masayoshi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4166-e0af188f094c195efd052d066e72cb40bf3ec66b714d5a7e08a0d91c2012332c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>current decay model</topic><topic>disruption</topic><topic>high βp plasma discharge</topic><topic>plasma inductance</topic><topic>poloidal beta</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>SHIBATA, Yoshihide</creatorcontrib><creatorcontrib>WATANABE, Kiyomasa</creatorcontrib><creatorcontrib>OHNO, Noriyasu</creatorcontrib><creatorcontrib>OKAMOTO, Masaaki</creatorcontrib><creatorcontrib>ISAYAMA, Akihiko</creatorcontrib><creatorcontrib>KURIHARA, Kenichi</creatorcontrib><creatorcontrib>OYAMA, Naoyuki</creatorcontrib><creatorcontrib>NAKANO, Tomohide</creatorcontrib><creatorcontrib>KAWANO, Yasunori</creatorcontrib><creatorcontrib>MATSUNAGA, Go</creatorcontrib><creatorcontrib>KAMADA, Yutaka</creatorcontrib><creatorcontrib>SUGIHARA, Masayoshi</creatorcontrib><collection>CrossRef</collection><jtitle>Plasma and Fusion Research</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>SHIBATA, Yoshihide</au><au>WATANABE, Kiyomasa</au><au>OHNO, Noriyasu</au><au>OKAMOTO, Masaaki</au><au>ISAYAMA, Akihiko</au><au>KURIHARA, Kenichi</au><au>OYAMA, Naoyuki</au><au>NAKANO, Tomohide</au><au>KAWANO, Yasunori</au><au>MATSUNAGA, Go</au><au>KAMADA, Yutaka</au><au>SUGIHARA, Masayoshi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Study of Plasma Current Decay in the Initial Phase of High Poloidal Beta Disruptions in JT-60U</atitle><jtitle>Plasma and Fusion Research</jtitle><addtitle>Plasma and Fusion Research</addtitle><date>2011</date><risdate>2011</risdate><volume>6</volume><spage>1302136</spage><epage>1302136</epage><pages>1302136-1302136</pages><issn>1880-6821</issn><eissn>1880-6821</eissn><abstract>In order to validate some current decay models during the current quench, the plasma current decay time was studied using the experimental plasma resistance and inductance in high poloidal beta, βp, disruptions in JT-60U. The plasma resistance and inductance were evaluated from an equilibrium calculation code and the measurement value of a magnetic sensor, the electron temperature evaluated by using ECE measurement and the electron density measured by FIR interferometer. In high βp disruptions, it was found that the electron temperature at the plasma center just after current quench starts was approximately 1-4 keV under almost the same current decay time observed during the initial phase of current quench. This result indicates that the electron temperature itself plays no major role in the determination of the current decay time in the initial phase of current quench. Moreover, the current decay time predicted by a modified L/R model [Y. Shibata et al., Nucl. Fusion 50, 025015 (2010)], in which the time derivative of plasma inductance was considered, was in good agreement with the experimental current decay time, while the values obtained from the conventional L/R model were two orders of magnitude larger than the experimental results.</abstract><pub>The Japan Society of Plasma Science and Nuclear Fusion Research</pub><doi>10.1585/pfr.6.1302136</doi><tpages>1</tpages><oa>free_for_read</oa></addata></record> |
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subjects | current decay model disruption high βp plasma discharge plasma inductance poloidal beta |
title | Study of Plasma Current Decay in the Initial Phase of High Poloidal Beta Disruptions in JT-60U |
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