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Superconducting strand properties at each production stage of the CMS solenoid conductor manufacturing
The Compact Muon Solenoid (CMS) detector is one of the general-purpose particle detectors presently being built for the LHC project at CERN. The superconducting CMS solenoid will produce a magnetic field of 4 T in a bore 6 m in diameter and 12.5 m long. The coil is wound from 20 high purity aluminum...
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Published in: | IEEE transactions on applied superconductivity 2004-06, Vol.14 (2), p.548-551 |
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container_title | IEEE transactions on applied superconductivity |
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creator | Blau, B. Campi, D. Cure, B. Greco, M. Kircher, F. Liikamaa, R. Seppala, J. Smith, R. Vieillard, L. |
description | The Compact Muon Solenoid (CMS) detector is one of the general-purpose particle detectors presently being built for the LHC project at CERN. The superconducting CMS solenoid will produce a magnetic field of 4 T in a bore 6 m in diameter and 12.5 m long. The coil is wound from 20 high purity aluminum-stabilized NbTi conductors with a total length of 45 km. The main part of the structural integrity of the CMS coil is ensured by aluminum-alloy reinforcement welded to the high purity aluminum stabilizer of the conductor. The Rutherford type superconducting cable within the stabilizer consists of 32 copper-stabilized multifilamentary NbTi strands each with Nb barrier. The strands are optimized with respect to a high critical current density (> 3000 A/mm/sup 2/ at 5 T, 4.2 K). Approximately 1950 km of superconducting strand has been produced from 148 extrusion billets and cabled in unit lengths of 2.65 km. All strands within a cable can unambiguously be identified by distinctive patterns of the NbTi filaments. The statistics of I/sub c/ measurements, n-value, copper RRR and (Cu + Nb)/NbTi ratio are presented. Since the strands are subjected to potentially dangerous high temperatures and mechanical strain during the different conductor production steps it was important to trace the critical current properties of the strand as it progressed through the conductor fabrication process. The paper presents results of I/sub c/ measurements, which were performed on all individual strands extracted from conductor samples taken at each step of the manufacturing process. The comparison among the measurements assured accurate quality control during the whole process of conductor production. In addition, I/sub c/ measurements in fields up to 6 T on the complete CMS conductors using the MaRiSA test facility are reported. |
doi_str_mv | 10.1109/TASC.2004.829716 |
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The superconducting CMS solenoid will produce a magnetic field of 4 T in a bore 6 m in diameter and 12.5 m long. The coil is wound from 20 high purity aluminum-stabilized NbTi conductors with a total length of 45 km. The main part of the structural integrity of the CMS coil is ensured by aluminum-alloy reinforcement welded to the high purity aluminum stabilizer of the conductor. The Rutherford type superconducting cable within the stabilizer consists of 32 copper-stabilized multifilamentary NbTi strands each with Nb barrier. The strands are optimized with respect to a high critical current density (> 3000 A/mm/sup 2/ at 5 T, 4.2 K). Approximately 1950 km of superconducting strand has been produced from 148 extrusion billets and cabled in unit lengths of 2.65 km. All strands within a cable can unambiguously be identified by distinctive patterns of the NbTi filaments. The statistics of I/sub c/ measurements, n-value, copper RRR and (Cu + Nb)/NbTi ratio are presented. Since the strands are subjected to potentially dangerous high temperatures and mechanical strain during the different conductor production steps it was important to trace the critical current properties of the strand as it progressed through the conductor fabrication process. The paper presents results of I/sub c/ measurements, which were performed on all individual strands extracted from conductor samples taken at each step of the manufacturing process. The comparison among the measurements assured accurate quality control during the whole process of conductor production. In addition, I/sub c/ measurements in fields up to 6 T on the complete CMS conductors using the MaRiSA test facility are reported.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2004.829716</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Aluminum ; Applied sciences ; Coiling ; Collision mitigation ; Conductors ; Conductors (devices) ; Cyclic accelerators and storage rings ; Detectors ; Electric connection. Cables. Wiring ; Electrical engineering. Electrical power engineering ; Exact sciences and technology ; Experimental methods and instrumentation for elementary-particle and nuclear physics ; High temperature superconductors ; Manufacturing ; Multifilamentary superconductors ; Niobium base alloys ; Niobium compounds ; Nuclear physics ; Physics ; Production ; Solenoids ; Strands ; Studies ; Superconducting cables ; Superconductivity ; Titanium compounds ; Various equipment and components</subject><ispartof>IEEE transactions on applied superconductivity, 2004-06, Vol.14 (2), p.548-551</ispartof><rights>2004 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2004</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c489t-c48b1e381eff4fa462eb087f4badb693d32e949d798568aff089ada1f17ee3cf3</citedby><cites>FETCH-LOGICAL-c489t-c48b1e381eff4fa462eb087f4badb693d32e949d798568aff089ada1f17ee3cf3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1324852$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>309,310,314,776,780,785,786,23909,23910,25118,27901,27902,54771</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=16197868$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Blau, B.</creatorcontrib><creatorcontrib>Campi, D.</creatorcontrib><creatorcontrib>Cure, B.</creatorcontrib><creatorcontrib>Greco, M.</creatorcontrib><creatorcontrib>Kircher, F.</creatorcontrib><creatorcontrib>Liikamaa, R.</creatorcontrib><creatorcontrib>Seppala, J.</creatorcontrib><creatorcontrib>Smith, R.</creatorcontrib><creatorcontrib>Vieillard, L.</creatorcontrib><title>Superconducting strand properties at each production stage of the CMS solenoid conductor manufacturing</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>The Compact Muon Solenoid (CMS) detector is one of the general-purpose particle detectors presently being built for the LHC project at CERN. The superconducting CMS solenoid will produce a magnetic field of 4 T in a bore 6 m in diameter and 12.5 m long. The coil is wound from 20 high purity aluminum-stabilized NbTi conductors with a total length of 45 km. The main part of the structural integrity of the CMS coil is ensured by aluminum-alloy reinforcement welded to the high purity aluminum stabilizer of the conductor. The Rutherford type superconducting cable within the stabilizer consists of 32 copper-stabilized multifilamentary NbTi strands each with Nb barrier. The strands are optimized with respect to a high critical current density (> 3000 A/mm/sup 2/ at 5 T, 4.2 K). Approximately 1950 km of superconducting strand has been produced from 148 extrusion billets and cabled in unit lengths of 2.65 km. All strands within a cable can unambiguously be identified by distinctive patterns of the NbTi filaments. The statistics of I/sub c/ measurements, n-value, copper RRR and (Cu + Nb)/NbTi ratio are presented. Since the strands are subjected to potentially dangerous high temperatures and mechanical strain during the different conductor production steps it was important to trace the critical current properties of the strand as it progressed through the conductor fabrication process. The paper presents results of I/sub c/ measurements, which were performed on all individual strands extracted from conductor samples taken at each step of the manufacturing process. The comparison among the measurements assured accurate quality control during the whole process of conductor production. In addition, I/sub c/ measurements in fields up to 6 T on the complete CMS conductors using the MaRiSA test facility are reported.</description><subject>Aluminum</subject><subject>Applied sciences</subject><subject>Coiling</subject><subject>Collision mitigation</subject><subject>Conductors</subject><subject>Conductors (devices)</subject><subject>Cyclic accelerators and storage rings</subject><subject>Detectors</subject><subject>Electric connection. Cables. Wiring</subject><subject>Electrical engineering. 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The superconducting CMS solenoid will produce a magnetic field of 4 T in a bore 6 m in diameter and 12.5 m long. The coil is wound from 20 high purity aluminum-stabilized NbTi conductors with a total length of 45 km. The main part of the structural integrity of the CMS coil is ensured by aluminum-alloy reinforcement welded to the high purity aluminum stabilizer of the conductor. The Rutherford type superconducting cable within the stabilizer consists of 32 copper-stabilized multifilamentary NbTi strands each with Nb barrier. The strands are optimized with respect to a high critical current density (> 3000 A/mm/sup 2/ at 5 T, 4.2 K). Approximately 1950 km of superconducting strand has been produced from 148 extrusion billets and cabled in unit lengths of 2.65 km. All strands within a cable can unambiguously be identified by distinctive patterns of the NbTi filaments. The statistics of I/sub c/ measurements, n-value, copper RRR and (Cu + Nb)/NbTi ratio are presented. Since the strands are subjected to potentially dangerous high temperatures and mechanical strain during the different conductor production steps it was important to trace the critical current properties of the strand as it progressed through the conductor fabrication process. The paper presents results of I/sub c/ measurements, which were performed on all individual strands extracted from conductor samples taken at each step of the manufacturing process. The comparison among the measurements assured accurate quality control during the whole process of conductor production. In addition, I/sub c/ measurements in fields up to 6 T on the complete CMS conductors using the MaRiSA test facility are reported.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TASC.2004.829716</doi><tpages>4</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Aluminum Applied sciences Coiling Collision mitigation Conductors Conductors (devices) Cyclic accelerators and storage rings Detectors Electric connection. Cables. Wiring Electrical engineering. Electrical power engineering Exact sciences and technology Experimental methods and instrumentation for elementary-particle and nuclear physics High temperature superconductors Manufacturing Multifilamentary superconductors Niobium base alloys Niobium compounds Nuclear physics Physics Production Solenoids Strands Studies Superconducting cables Superconductivity Titanium compounds Various equipment and components |
title | Superconducting strand properties at each production stage of the CMS solenoid conductor manufacturing |
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