Characteristics of Cu Stabilized Strands With Low Cu Ratio
Characteristics of recently developed F4-Nb 3 Al strand with low Cu ratio are described. The overall J c of the Nb 3 Al strand could be easily increased by decreasing of the Cu ratio. Although the quench of a pulse-like voltage generation is usually observed in superconducting unstable conductor, th...
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Veröffentlicht in: | IEEE transactions on applied superconductivity 2009-06, Vol.19 (3), p.2678-2681 |
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creator | Kikuchi, A. Yamada, R. Barzi, E. Kobayashi, M. Lamm, M. Nakagawa, K. Sasaki, K.-i. Takeuchi, T. Turrioni, D. Zlobin, A.V. |
description | Characteristics of recently developed F4-Nb 3 Al strand with low Cu ratio are described. The overall J c of the Nb 3 Al strand could be easily increased by decreasing of the Cu ratio. Although the quench of a pulse-like voltage generation is usually observed in superconducting unstable conductor, the F4 strand with a low Cu ratio of 0.61 exhibited an ordinary critical transition of gradual voltage generation. The F4 strand does not have magnetic instabilities at 4.2 K because of the tantalum interfilament matrix. The overall J c of the F4 strand achieved was 80-85% of the RRP strand. In the large mechanical stress above 100 MPa, the overall J c of the F4 strand might be comparable to that of high J c RRP-Nb 3 Sn strands. The Rutherford cable with a high packing factor of 86.5% has been fabricated using F4 strands. The small racetrack magnet, SR07, was also fabricated by a 14 m F4 cable. The quench current, I q , of SR07 were obtained 22.4 kA at 4.5 K and 25.2 kA at 2.2 K. The tantalum matrix Nb 3 Al strands are promising for the application of super-cooled high-field magnets as well as 4.2 K operation magnets. |
doi_str_mv | 10.1109/TASC.2009.2018303 |
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The overall J c of the Nb 3 Al strand could be easily increased by decreasing of the Cu ratio. Although the quench of a pulse-like voltage generation is usually observed in superconducting unstable conductor, the F4 strand with a low Cu ratio of 0.61 exhibited an ordinary critical transition of gradual voltage generation. The F4 strand does not have magnetic instabilities at 4.2 K because of the tantalum interfilament matrix. The overall J c of the F4 strand achieved was 80-85% of the RRP strand. In the large mechanical stress above 100 MPa, the overall J c of the F4 strand might be comparable to that of high J c RRP-Nb 3 Sn strands. The Rutherford cable with a high packing factor of 86.5% has been fabricated using F4 strands. The small racetrack magnet, SR07, was also fabricated by a 14 m F4 cable. The quench current, I q , of SR07 were obtained 22.4 kA at 4.5 K and 25.2 kA at 2.2 K. The tantalum matrix Nb 3 Al strands are promising for the application of super-cooled high-field magnets as well as 4.2 K operation magnets.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2009.2018303</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Copper ; Copper stabilizer ; Critical current ; Degradation ; Magnetic separation ; magnetization ; Materials science and technology ; Pulse generation ; Rutherford cable ; small racetrack magnet ; Stress ; Superconducting magnets ; Testing ; Voltage ; {\rm Nb}_{3}{\rm Al} strand</subject><ispartof>IEEE transactions on applied superconductivity, 2009-06, Vol.19 (3), p.2678-2681</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2009</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1373-c7d0f5ad99a34eec8e5d5fb03829f283ba70e3c14f76d04847f65b7102f31c6e3</citedby><cites>FETCH-LOGICAL-c1373-c7d0f5ad99a34eec8e5d5fb03829f283ba70e3c14f76d04847f65b7102f31c6e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/5153175$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/5153175$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Kikuchi, A.</creatorcontrib><creatorcontrib>Yamada, R.</creatorcontrib><creatorcontrib>Barzi, E.</creatorcontrib><creatorcontrib>Kobayashi, M.</creatorcontrib><creatorcontrib>Lamm, M.</creatorcontrib><creatorcontrib>Nakagawa, K.</creatorcontrib><creatorcontrib>Sasaki, K.-i.</creatorcontrib><creatorcontrib>Takeuchi, T.</creatorcontrib><creatorcontrib>Turrioni, D.</creatorcontrib><creatorcontrib>Zlobin, A.V.</creatorcontrib><title>Characteristics of Cu Stabilized Strands With Low Cu Ratio</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>Characteristics of recently developed F4-Nb 3 Al strand with low Cu ratio are described. The overall J c of the Nb 3 Al strand could be easily increased by decreasing of the Cu ratio. Although the quench of a pulse-like voltage generation is usually observed in superconducting unstable conductor, the F4 strand with a low Cu ratio of 0.61 exhibited an ordinary critical transition of gradual voltage generation. The F4 strand does not have magnetic instabilities at 4.2 K because of the tantalum interfilament matrix. The overall J c of the F4 strand achieved was 80-85% of the RRP strand. In the large mechanical stress above 100 MPa, the overall J c of the F4 strand might be comparable to that of high J c RRP-Nb 3 Sn strands. The Rutherford cable with a high packing factor of 86.5% has been fabricated using F4 strands. The small racetrack magnet, SR07, was also fabricated by a 14 m F4 cable. The quench current, I q , of SR07 were obtained 22.4 kA at 4.5 K and 25.2 kA at 2.2 K. The tantalum matrix Nb 3 Al strands are promising for the application of super-cooled high-field magnets as well as 4.2 K operation magnets.</description><subject>Copper</subject><subject>Copper stabilizer</subject><subject>Critical current</subject><subject>Degradation</subject><subject>Magnetic separation</subject><subject>magnetization</subject><subject>Materials science and technology</subject><subject>Pulse generation</subject><subject>Rutherford cable</subject><subject>small racetrack magnet</subject><subject>Stress</subject><subject>Superconducting magnets</subject><subject>Testing</subject><subject>Voltage</subject><subject>{\rm Nb}_{3}{\rm Al} strand</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kE9LAzEQxYMoWKsfQLws3rfOJJtN1ltZ_AcLgq14DNlsQlNqtyZbRD-9WVq8zAzMe_OGHyHXCDNEqO6W80U9owBVKigZsBMyQc5lTjny0zQDx1xSys7JRYxrACxkwSfkvl7poM1gg4-DNzHrXVbvs8WgW7_xv7ZLY9DbLmYfflhlTf89rt_04PtLcub0JtqrY5-S98eHZf2cN69PL_W8yQ0ywXIjOnBcd1WlWWGtkZZ33LXAJK0clazVAiwzWDhRdpC-Eq7krUCgjqEpLZuS28PdXei_9jYOat3vwzZFqgoplJBSkggPIhP6GIN1ahf8pw4_CkGNhNRISI2E1JFQ8twcPN5a-69PvBgKzv4AnkBgIA</recordid><startdate>200906</startdate><enddate>200906</enddate><creator>Kikuchi, A.</creator><creator>Yamada, R.</creator><creator>Barzi, E.</creator><creator>Kobayashi, M.</creator><creator>Lamm, M.</creator><creator>Nakagawa, K.</creator><creator>Sasaki, K.-i.</creator><creator>Takeuchi, T.</creator><creator>Turrioni, D.</creator><creator>Zlobin, A.V.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>200906</creationdate><title>Characteristics of Cu Stabilized Strands With Low Cu Ratio</title><author>Kikuchi, A. ; Yamada, R. ; Barzi, E. ; Kobayashi, M. ; Lamm, M. ; Nakagawa, K. ; Sasaki, K.-i. ; Takeuchi, T. ; Turrioni, D. ; Zlobin, A.V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1373-c7d0f5ad99a34eec8e5d5fb03829f283ba70e3c14f76d04847f65b7102f31c6e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2009</creationdate><topic>Copper</topic><topic>Copper stabilizer</topic><topic>Critical current</topic><topic>Degradation</topic><topic>Magnetic separation</topic><topic>magnetization</topic><topic>Materials science and technology</topic><topic>Pulse generation</topic><topic>Rutherford cable</topic><topic>small racetrack magnet</topic><topic>Stress</topic><topic>Superconducting magnets</topic><topic>Testing</topic><topic>Voltage</topic><topic>{\rm Nb}_{3}{\rm Al} strand</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kikuchi, A.</creatorcontrib><creatorcontrib>Yamada, R.</creatorcontrib><creatorcontrib>Barzi, E.</creatorcontrib><creatorcontrib>Kobayashi, M.</creatorcontrib><creatorcontrib>Lamm, M.</creatorcontrib><creatorcontrib>Nakagawa, K.</creatorcontrib><creatorcontrib>Sasaki, K.-i.</creatorcontrib><creatorcontrib>Takeuchi, T.</creatorcontrib><creatorcontrib>Turrioni, D.</creatorcontrib><creatorcontrib>Zlobin, A.V.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology 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_linktorsrc</fulltext></delivery><addata><au>Kikuchi, A.</au><au>Yamada, R.</au><au>Barzi, E.</au><au>Kobayashi, M.</au><au>Lamm, M.</au><au>Nakagawa, K.</au><au>Sasaki, K.-i.</au><au>Takeuchi, T.</au><au>Turrioni, D.</au><au>Zlobin, A.V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Characteristics of Cu Stabilized Strands With Low Cu Ratio</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><stitle>TASC</stitle><date>2009-06</date><risdate>2009</risdate><volume>19</volume><issue>3</issue><spage>2678</spage><epage>2681</epage><pages>2678-2681</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><coden>ITASE9</coden><abstract>Characteristics of recently developed F4-Nb 3 Al strand with low Cu ratio are described. The overall J c of the Nb 3 Al strand could be easily increased by decreasing of the Cu ratio. Although the quench of a pulse-like voltage generation is usually observed in superconducting unstable conductor, the F4 strand with a low Cu ratio of 0.61 exhibited an ordinary critical transition of gradual voltage generation. The F4 strand does not have magnetic instabilities at 4.2 K because of the tantalum interfilament matrix. The overall J c of the F4 strand achieved was 80-85% of the RRP strand. In the large mechanical stress above 100 MPa, the overall J c of the F4 strand might be comparable to that of high J c RRP-Nb 3 Sn strands. The Rutherford cable with a high packing factor of 86.5% has been fabricated using F4 strands. The small racetrack magnet, SR07, was also fabricated by a 14 m F4 cable. The quench current, I q , of SR07 were obtained 22.4 kA at 4.5 K and 25.2 kA at 2.2 K. The tantalum matrix Nb 3 Al strands are promising for the application of super-cooled high-field magnets as well as 4.2 K operation magnets.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TASC.2009.2018303</doi><tpages>4</tpages></addata></record> |
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subjects | Copper Copper stabilizer Critical current Degradation Magnetic separation magnetization Materials science and technology Pulse generation Rutherford cable small racetrack magnet Stress Superconducting magnets Testing Voltage {\rm Nb}_{3}{\rm Al} strand |
title | Characteristics of Cu Stabilized Strands With Low Cu Ratio |
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