Fabrication and Characteristics of 2G HTS Current Leads
2nd generation high temperature superconducting (2G-HTS) tape consists of multi-layers such substrate, buffer layer, superconducting layer and reinforced lamination tapes. 2G HTS tape is a candidate of good materials for current lead of superconducting magnet system owing to its low thermal conducti...
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Veröffentlicht in: | IEEE transactions on applied superconductivity 2010-06, Vol.20 (3), p.1755-1758 |
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container_title | IEEE transactions on applied superconductivity |
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creator | SOHN, Myung-Hwan KIM, Seokho SIM, Kideok BAE, Joon-Han LEE, Seok-Ju PARK, Hae-Yong |
description | 2nd generation high temperature superconducting (2G-HTS) tape consists of multi-layers such substrate, buffer layer, superconducting layer and reinforced lamination tapes. 2G HTS tape is a candidate of good materials for current lead of superconducting magnet system owing to its low thermal conductivity. However, joint resistance between 2G HTS tapes and terminal block can be a major problem because of high electrical resistivity of substrate, buffer layer and reinforced lamination tapes of 2G HTS. So specially considering joint resistance between 2G tapes and terminal block, 2G HTS current lead for 400 A was designed and fabricated. This current lead was consisting of two terminal blocks, a support bar or tube, protection tube and six 2G HTS tapes. Its total length was 300 mm and body diameter 18.3 mm. At liquid nitrogen temperature (77 K) critical current (Ic) of this HTS current lead was 600 A, about 1.5 times the operating current 400 A. Conductive heat loss of 2G HTS current lead between 60 K and 7 K was 50 mW. |
doi_str_mv | 10.1109/TASC.2010.2042588 |
format | Article |
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However, joint resistance between 2G HTS tapes and terminal block can be a major problem because of high electrical resistivity of substrate, buffer layer and reinforced lamination tapes of 2G HTS. So specially considering joint resistance between 2G tapes and terminal block, 2G HTS current lead for 400 A was designed and fabricated. This current lead was consisting of two terminal blocks, a support bar or tube, protection tube and six 2G HTS tapes. Its total length was 300 mm and body diameter 18.3 mm. At liquid nitrogen temperature (77 K) critical current (Ic) of this HTS current lead was 600 A, about 1.5 times the operating current 400 A. Conductive heat loss of 2G HTS current lead between 60 K and 7 K was 50 mW.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2010.2042588</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>2G HTS tape ; Applied sciences ; Blocking ; Buffer layers ; Current lead ; Electric connection. Cables. Wiring ; Electric resistance ; Electrical engineering. Electrical power engineering ; Electromagnets ; Electronics ; Exact sciences and technology ; Fabrication ; High temperature superconductors ; joint resistance ; Laminates ; Lamination ; Magnetic materials ; Materials ; Multilayers ; R&D ; Research & development ; Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices ; Superconducting devices ; Superconducting epitaxial layers ; Superconducting films ; Superconducting magnets ; Superconducting materials ; Superconducting tapes ; Superconductivity ; Terminals ; thermal conductivity ; Tubes ; Various equipment and components</subject><ispartof>IEEE transactions on applied superconductivity, 2010-06, Vol.20 (3), p.1755-1758</ispartof><rights>2015 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) Jun 2010</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c355t-c9ebb3e32d7a42febfc0cc52202d311b1ea904a47182e062ce3a2c95da2211b03</citedby><cites>FETCH-LOGICAL-c355t-c9ebb3e32d7a42febfc0cc52202d311b1ea904a47182e062ce3a2c95da2211b03</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/5424101$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>309,310,314,776,780,785,786,792,23911,23912,25120,27903,27904,54736</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/5424101$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=22862876$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>SOHN, Myung-Hwan</creatorcontrib><creatorcontrib>KIM, Seokho</creatorcontrib><creatorcontrib>SIM, Kideok</creatorcontrib><creatorcontrib>BAE, Joon-Han</creatorcontrib><creatorcontrib>LEE, Seok-Ju</creatorcontrib><creatorcontrib>PARK, Hae-Yong</creatorcontrib><title>Fabrication and Characteristics of 2G HTS Current Leads</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>2nd generation high temperature superconducting (2G-HTS) tape consists of multi-layers such substrate, buffer layer, superconducting layer and reinforced lamination tapes. 2G HTS tape is a candidate of good materials for current lead of superconducting magnet system owing to its low thermal conductivity. However, joint resistance between 2G HTS tapes and terminal block can be a major problem because of high electrical resistivity of substrate, buffer layer and reinforced lamination tapes of 2G HTS. So specially considering joint resistance between 2G tapes and terminal block, 2G HTS current lead for 400 A was designed and fabricated. This current lead was consisting of two terminal blocks, a support bar or tube, protection tube and six 2G HTS tapes. Its total length was 300 mm and body diameter 18.3 mm. At liquid nitrogen temperature (77 K) critical current (Ic) of this HTS current lead was 600 A, about 1.5 times the operating current 400 A. Conductive heat loss of 2G HTS current lead between 60 K and 7 K was 50 mW.</description><subject>2G HTS tape</subject><subject>Applied sciences</subject><subject>Blocking</subject><subject>Buffer layers</subject><subject>Current lead</subject><subject>Electric connection. Cables. Wiring</subject><subject>Electric resistance</subject><subject>Electrical engineering. Electrical power engineering</subject><subject>Electromagnets</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>Fabrication</subject><subject>High temperature superconductors</subject><subject>joint resistance</subject><subject>Laminates</subject><subject>Lamination</subject><subject>Magnetic materials</subject><subject>Materials</subject><subject>Multilayers</subject><subject>R&D</subject><subject>Research & development</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</subject><subject>Superconducting devices</subject><subject>Superconducting epitaxial layers</subject><subject>Superconducting films</subject><subject>Superconducting magnets</subject><subject>Superconducting materials</subject><subject>Superconducting tapes</subject><subject>Superconductivity</subject><subject>Terminals</subject><subject>thermal conductivity</subject><subject>Tubes</subject><subject>Various equipment and components</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNpdkEFLw0AQhYMoWKs_QLwERDyl7s7uJpujBNsKBQ-t52WymeCWNKm7ycF_b2pLD55mhve9x_Ci6J6zGecsf9m8rosZsPEEJkFpfRFNuFI6AcXV5bgzxRMNIK6jmxC2jHGppZpE2RxL7yz2rmtjbKu4-EKPtifvQu9siLs6hkW83KzjYvCe2j5eEVbhNrqqsQl0d5rT6HP-timWyepj8V68rhIrlOoTm1NZChJQZSihprK2zFoFwKASnJecMGcSZcY1EEvBkkCwuaoQYJSZmEbPx9y9774HCr3ZuWCpabClbggmUyKDXGg1ko__yG03-HZ8znAGGTCV_lH8SFnfheCpNnvvduh_RsgcmjSHJs2hSXNqcvQ8nZIxWGxqj6114WwE0CnoLB25hyPniOgsKwmSMy5-AfGjeYM</recordid><startdate>20100601</startdate><enddate>20100601</enddate><creator>SOHN, Myung-Hwan</creator><creator>KIM, Seokho</creator><creator>SIM, Kideok</creator><creator>BAE, Joon-Han</creator><creator>LEE, Seok-Ju</creator><creator>PARK, Hae-Yong</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>F28</scope><scope>FR3</scope></search><sort><creationdate>20100601</creationdate><title>Fabrication and Characteristics of 2G HTS Current Leads</title><author>SOHN, Myung-Hwan ; KIM, Seokho ; SIM, Kideok ; BAE, Joon-Han ; LEE, Seok-Ju ; PARK, Hae-Yong</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c355t-c9ebb3e32d7a42febfc0cc52202d311b1ea904a47182e062ce3a2c95da2211b03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>2G HTS tape</topic><topic>Applied sciences</topic><topic>Blocking</topic><topic>Buffer layers</topic><topic>Current lead</topic><topic>Electric connection. Cables. Wiring</topic><topic>Electric resistance</topic><topic>Electrical engineering. Electrical power engineering</topic><topic>Electromagnets</topic><topic>Electronics</topic><topic>Exact sciences and technology</topic><topic>Fabrication</topic><topic>High temperature superconductors</topic><topic>joint resistance</topic><topic>Laminates</topic><topic>Lamination</topic><topic>Magnetic materials</topic><topic>Materials</topic><topic>Multilayers</topic><topic>R&D</topic><topic>Research & development</topic><topic>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</topic><topic>Superconducting devices</topic><topic>Superconducting epitaxial layers</topic><topic>Superconducting films</topic><topic>Superconducting magnets</topic><topic>Superconducting materials</topic><topic>Superconducting tapes</topic><topic>Superconductivity</topic><topic>Terminals</topic><topic>thermal conductivity</topic><topic>Tubes</topic><topic>Various equipment and components</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>SOHN, Myung-Hwan</creatorcontrib><creatorcontrib>KIM, Seokho</creatorcontrib><creatorcontrib>SIM, Kideok</creatorcontrib><creatorcontrib>BAE, Joon-Han</creatorcontrib><creatorcontrib>LEE, Seok-Ju</creatorcontrib><creatorcontrib>PARK, Hae-Yong</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>Pascal-Francis</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><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><jtitle>IEEE transactions on applied superconductivity</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>SOHN, Myung-Hwan</au><au>KIM, Seokho</au><au>SIM, Kideok</au><au>BAE, Joon-Han</au><au>LEE, Seok-Ju</au><au>PARK, Hae-Yong</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Fabrication and Characteristics of 2G HTS Current Leads</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><stitle>TASC</stitle><date>2010-06-01</date><risdate>2010</risdate><volume>20</volume><issue>3</issue><spage>1755</spage><epage>1758</epage><pages>1755-1758</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><coden>ITASE9</coden><abstract>2nd generation high temperature superconducting (2G-HTS) tape consists of multi-layers such substrate, buffer layer, superconducting layer and reinforced lamination tapes. 2G HTS tape is a candidate of good materials for current lead of superconducting magnet system owing to its low thermal conductivity. However, joint resistance between 2G HTS tapes and terminal block can be a major problem because of high electrical resistivity of substrate, buffer layer and reinforced lamination tapes of 2G HTS. So specially considering joint resistance between 2G tapes and terminal block, 2G HTS current lead for 400 A was designed and fabricated. This current lead was consisting of two terminal blocks, a support bar or tube, protection tube and six 2G HTS tapes. Its total length was 300 mm and body diameter 18.3 mm. At liquid nitrogen temperature (77 K) critical current (Ic) of this HTS current lead was 600 A, about 1.5 times the operating current 400 A. Conductive heat loss of 2G HTS current lead between 60 K and 7 K was 50 mW.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TASC.2010.2042588</doi><tpages>4</tpages></addata></record> |
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subjects | 2G HTS tape Applied sciences Blocking Buffer layers Current lead Electric connection. Cables. Wiring Electric resistance Electrical engineering. Electrical power engineering Electromagnets Electronics Exact sciences and technology Fabrication High temperature superconductors joint resistance Laminates Lamination Magnetic materials Materials Multilayers R&D Research & development Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices Superconducting devices Superconducting epitaxial layers Superconducting films Superconducting magnets Superconducting materials Superconducting tapes Superconductivity Terminals thermal conductivity Tubes Various equipment and components |
title | Fabrication and Characteristics of 2G HTS Current Leads |
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