Performance Analysis of Mass-Produced Nb sub(3)Sn Conductor for Central Solenoid in ITER
The performance of two mass-produced Nb sub(3)Sn conductors for the ITER central solenoids was tested for the first time. One was cut from the forward end of an 80-m-long conductor, and the other was cut from the forward end of a 918-m-long conductor. The fifth-stage twist pitches of these conductor...
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Veröffentlicht in: | IEEE transactions on applied superconductivity 2016-06, Vol.26 (4), p.1-5 |
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creator | Nabara, Yoshihiro Suwa, Tomone Ozeki, Hidemasa Kajitani, Hideki Sakurai, Takeru Hemmi, Tsutomu Iguchi, Masahide Nunoya, Yoshihiko Takahashi, Yoshikazu Isono, Takaaki Matsui, Kunihiro Koizumi, Norikiyo Tsutsumi, Fumiaki Uno, Yasuhiro Oshikiri, Masayuki Shibutani, Kazuyuki Okuno, Kiyoshi Murakami, Yukinobu Takano, Tsuyoshi Sedlak, Kamil Stepanov, Boris Bruzzone, Pierluigi |
description | The performance of two mass-produced Nb sub(3)Sn conductors for the ITER central solenoids was tested for the first time. One was cut from the forward end of an 80-m-long conductor, and the other was cut from the forward end of a 918-m-long conductor. The fifth-stage twist pitches of these conductors were lengthened by approximately 16% during cable insertion and compaction with conduit. The current sharing temperatures $T_{cs}$ were measured over 20 000 electromagnetic cycles, including four thermal cycles between 4.2 K and room temperature. The $T_{cs}$ of the former conductor increased and became almost constant through the cycling. In contrast, $T_{cs}$ of the latter conductor not only increased but also decreased slightly against cycling. The $T_{cs}$ decline rate after 10 002 cycles was $-4.50\times 10-6}\ \text{K/cycle}$. If this rate is assumed to continue after 20 000 cycles, $T_{cs}$ would decrease by -0.27 K over 60 000 cycles. Even so, $T_{cs}$ is higher than an acceptance criterion of 6.5 K at 60 000 cycles. The ac losses $Q$ of both conductors at a current of 0 kA were almost the same as or slightly lower than $Q$ of a short sample conductor whose fifth-stage twist pitch was not lengthen. On each conductor, $Q$ at 40 kA was approximately 10% higher than that at 0 kA; thus, the effect of the transport current on $Q$ was not large. |
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One was cut from the forward end of an 80-m-long conductor, and the other was cut from the forward end of a 918-m-long conductor. The fifth-stage twist pitches of these conductors were lengthened by approximately 16% during cable insertion and compaction with conduit. The current sharing temperatures $T_{cs}$ were measured over 20 000 electromagnetic cycles, including four thermal cycles between 4.2 K and room temperature. The $T_{cs}$ of the former conductor increased and became almost constant through the cycling. In contrast, $T_{cs}$ of the latter conductor not only increased but also decreased slightly against cycling. The $T_{cs}$ decline rate after 10 002 cycles was $-4.50\times 10-6}\ \text{K/cycle}$. If this rate is assumed to continue after 20 000 cycles, $T_{cs}$ would decrease by -0.27 K over 60 000 cycles. Even so, $T_{cs}$ is higher than an acceptance criterion of 6.5 K at 60 000 cycles. The ac losses $Q$ of both conductors at a current of 0 kA were almost the same as or slightly lower than $Q$ of a short sample conductor whose fifth-stage twist pitch was not lengthen. On each conductor, $Q$ at 40 kA was approximately 10% higher than that at 0 kA; thus, the effect of the transport current on $Q$ was not large.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2016.2518640</identifier><language>eng</language><subject>Conductors (devices) ; Conduits ; Constants ; Current sharing ; Cycles ; Insertion ; Solenoids ; Superconductivity</subject><ispartof>IEEE transactions on applied superconductivity, 2016-06, Vol.26 (4), p.1-5</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Nabara, Yoshihiro</creatorcontrib><creatorcontrib>Suwa, Tomone</creatorcontrib><creatorcontrib>Ozeki, Hidemasa</creatorcontrib><creatorcontrib>Kajitani, Hideki</creatorcontrib><creatorcontrib>Sakurai, Takeru</creatorcontrib><creatorcontrib>Hemmi, Tsutomu</creatorcontrib><creatorcontrib>Iguchi, Masahide</creatorcontrib><creatorcontrib>Nunoya, Yoshihiko</creatorcontrib><creatorcontrib>Takahashi, Yoshikazu</creatorcontrib><creatorcontrib>Isono, Takaaki</creatorcontrib><creatorcontrib>Matsui, Kunihiro</creatorcontrib><creatorcontrib>Koizumi, Norikiyo</creatorcontrib><creatorcontrib>Tsutsumi, Fumiaki</creatorcontrib><creatorcontrib>Uno, Yasuhiro</creatorcontrib><creatorcontrib>Oshikiri, Masayuki</creatorcontrib><creatorcontrib>Shibutani, Kazuyuki</creatorcontrib><creatorcontrib>Okuno, Kiyoshi</creatorcontrib><creatorcontrib>Murakami, Yukinobu</creatorcontrib><creatorcontrib>Takano, Tsuyoshi</creatorcontrib><creatorcontrib>Sedlak, Kamil</creatorcontrib><creatorcontrib>Stepanov, Boris</creatorcontrib><creatorcontrib>Bruzzone, Pierluigi</creatorcontrib><title>Performance Analysis of Mass-Produced Nb sub(3)Sn Conductor for Central Solenoid in ITER</title><title>IEEE transactions on applied superconductivity</title><description>The performance of two mass-produced Nb sub(3)Sn conductors for the ITER central solenoids was tested for the first time. One was cut from the forward end of an 80-m-long conductor, and the other was cut from the forward end of a 918-m-long conductor. The fifth-stage twist pitches of these conductors were lengthened by approximately 16% during cable insertion and compaction with conduit. The current sharing temperatures $T_{cs}$ were measured over 20 000 electromagnetic cycles, including four thermal cycles between 4.2 K and room temperature. The $T_{cs}$ of the former conductor increased and became almost constant through the cycling. In contrast, $T_{cs}$ of the latter conductor not only increased but also decreased slightly against cycling. The $T_{cs}$ decline rate after 10 002 cycles was $-4.50\times 10-6}\ \text{K/cycle}$. If this rate is assumed to continue after 20 000 cycles, $T_{cs}$ would decrease by -0.27 K over 60 000 cycles. Even so, $T_{cs}$ is higher than an acceptance criterion of 6.5 K at 60 000 cycles. The ac losses $Q$ of both conductors at a current of 0 kA were almost the same as or slightly lower than $Q$ of a short sample conductor whose fifth-stage twist pitch was not lengthen. On each conductor, $Q$ at 40 kA was approximately 10% higher than that at 0 kA; thus, the effect of the transport current on $Q$ was not large.</description><subject>Conductors (devices)</subject><subject>Conduits</subject><subject>Constants</subject><subject>Current sharing</subject><subject>Cycles</subject><subject>Insertion</subject><subject>Solenoids</subject><subject>Superconductivity</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqVi7FOw0AQRE8IJELgA-i2DIXN3dkbjjKygkIBimIXdNHFXktGl1u4tQv-Hhf8ANXMG71R6t7o3Bj9_Nhs6iq32qxzi8atS32hFgbRZTPi5dw1msxZW1yrG5FPrU3pSlyojz2lntPZx5ZgE334kUGAe3jzItk-cTe11MH7CWQ6rYqHOkLFcR5HTjAfoaI4Jh-g5kCRhw6GCK_N9nCrrnofhO7-cqlWL9um2mVfib8nkvF4HqSlEHwknuRonEV80uhs8Q_1F9QNSws</recordid><startdate>20160601</startdate><enddate>20160601</enddate><creator>Nabara, Yoshihiro</creator><creator>Suwa, Tomone</creator><creator>Ozeki, Hidemasa</creator><creator>Kajitani, Hideki</creator><creator>Sakurai, Takeru</creator><creator>Hemmi, Tsutomu</creator><creator>Iguchi, Masahide</creator><creator>Nunoya, Yoshihiko</creator><creator>Takahashi, Yoshikazu</creator><creator>Isono, Takaaki</creator><creator>Matsui, Kunihiro</creator><creator>Koizumi, Norikiyo</creator><creator>Tsutsumi, Fumiaki</creator><creator>Uno, Yasuhiro</creator><creator>Oshikiri, Masayuki</creator><creator>Shibutani, Kazuyuki</creator><creator>Okuno, Kiyoshi</creator><creator>Murakami, Yukinobu</creator><creator>Takano, Tsuyoshi</creator><creator>Sedlak, Kamil</creator><creator>Stepanov, Boris</creator><creator>Bruzzone, Pierluigi</creator><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>L7M</scope></search><sort><creationdate>20160601</creationdate><title>Performance Analysis of Mass-Produced Nb sub(3)Sn Conductor for Central Solenoid in ITER</title><author>Nabara, Yoshihiro ; Suwa, Tomone ; Ozeki, Hidemasa ; Kajitani, Hideki ; Sakurai, Takeru ; Hemmi, Tsutomu ; Iguchi, Masahide ; Nunoya, Yoshihiko ; Takahashi, Yoshikazu ; Isono, Takaaki ; Matsui, Kunihiro ; Koizumi, Norikiyo ; Tsutsumi, Fumiaki ; Uno, Yasuhiro ; Oshikiri, Masayuki ; Shibutani, Kazuyuki ; Okuno, Kiyoshi ; Murakami, Yukinobu ; Takano, Tsuyoshi ; Sedlak, Kamil ; Stepanov, Boris ; Bruzzone, Pierluigi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_18255705823</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Conductors (devices)</topic><topic>Conduits</topic><topic>Constants</topic><topic>Current sharing</topic><topic>Cycles</topic><topic>Insertion</topic><topic>Solenoids</topic><topic>Superconductivity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nabara, Yoshihiro</creatorcontrib><creatorcontrib>Suwa, Tomone</creatorcontrib><creatorcontrib>Ozeki, Hidemasa</creatorcontrib><creatorcontrib>Kajitani, Hideki</creatorcontrib><creatorcontrib>Sakurai, Takeru</creatorcontrib><creatorcontrib>Hemmi, Tsutomu</creatorcontrib><creatorcontrib>Iguchi, Masahide</creatorcontrib><creatorcontrib>Nunoya, Yoshihiko</creatorcontrib><creatorcontrib>Takahashi, Yoshikazu</creatorcontrib><creatorcontrib>Isono, Takaaki</creatorcontrib><creatorcontrib>Matsui, Kunihiro</creatorcontrib><creatorcontrib>Koizumi, Norikiyo</creatorcontrib><creatorcontrib>Tsutsumi, Fumiaki</creatorcontrib><creatorcontrib>Uno, Yasuhiro</creatorcontrib><creatorcontrib>Oshikiri, Masayuki</creatorcontrib><creatorcontrib>Shibutani, Kazuyuki</creatorcontrib><creatorcontrib>Okuno, Kiyoshi</creatorcontrib><creatorcontrib>Murakami, Yukinobu</creatorcontrib><creatorcontrib>Takano, Tsuyoshi</creatorcontrib><creatorcontrib>Sedlak, Kamil</creatorcontrib><creatorcontrib>Stepanov, Boris</creatorcontrib><creatorcontrib>Bruzzone, Pierluigi</creatorcontrib><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>IEEE transactions on applied superconductivity</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nabara, Yoshihiro</au><au>Suwa, Tomone</au><au>Ozeki, Hidemasa</au><au>Kajitani, Hideki</au><au>Sakurai, Takeru</au><au>Hemmi, Tsutomu</au><au>Iguchi, Masahide</au><au>Nunoya, Yoshihiko</au><au>Takahashi, Yoshikazu</au><au>Isono, Takaaki</au><au>Matsui, Kunihiro</au><au>Koizumi, Norikiyo</au><au>Tsutsumi, Fumiaki</au><au>Uno, Yasuhiro</au><au>Oshikiri, Masayuki</au><au>Shibutani, Kazuyuki</au><au>Okuno, Kiyoshi</au><au>Murakami, Yukinobu</au><au>Takano, Tsuyoshi</au><au>Sedlak, Kamil</au><au>Stepanov, Boris</au><au>Bruzzone, Pierluigi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Performance Analysis of Mass-Produced Nb sub(3)Sn Conductor for Central Solenoid in ITER</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><date>2016-06-01</date><risdate>2016</risdate><volume>26</volume><issue>4</issue><spage>1</spage><epage>5</epage><pages>1-5</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><abstract>The performance of two mass-produced Nb sub(3)Sn conductors for the ITER central solenoids was tested for the first time. One was cut from the forward end of an 80-m-long conductor, and the other was cut from the forward end of a 918-m-long conductor. The fifth-stage twist pitches of these conductors were lengthened by approximately 16% during cable insertion and compaction with conduit. The current sharing temperatures $T_{cs}$ were measured over 20 000 electromagnetic cycles, including four thermal cycles between 4.2 K and room temperature. The $T_{cs}$ of the former conductor increased and became almost constant through the cycling. In contrast, $T_{cs}$ of the latter conductor not only increased but also decreased slightly against cycling. The $T_{cs}$ decline rate after 10 002 cycles was $-4.50\times 10-6}\ \text{K/cycle}$. If this rate is assumed to continue after 20 000 cycles, $T_{cs}$ would decrease by -0.27 K over 60 000 cycles. Even so, $T_{cs}$ is higher than an acceptance criterion of 6.5 K at 60 000 cycles. The ac losses $Q$ of both conductors at a current of 0 kA were almost the same as or slightly lower than $Q$ of a short sample conductor whose fifth-stage twist pitch was not lengthen. On each conductor, $Q$ at 40 kA was approximately 10% higher than that at 0 kA; thus, the effect of the transport current on $Q$ was not large.</abstract><doi>10.1109/TASC.2016.2518640</doi></addata></record> |
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subjects | Conductors (devices) Conduits Constants Current sharing Cycles Insertion Solenoids Superconductivity |
title | Performance Analysis of Mass-Produced Nb sub(3)Sn Conductor for Central Solenoid in ITER |
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