Influence of Field Direction and Conductor Aspect Ratio on Coupling Losses: Measurements and Modeling on the JT-60SA TF Conductor
AC losses induced by magnetic field variations dissipate power in the conductors of coils during the tokamak operation. They can be critical for being a possible source of resistive transitions and leading to a possible quench in the magnet. This paper aims at presenting the results of the influence...
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Veröffentlicht in: | IEEE transactions on applied superconductivity 2024-08, Vol.34 (5), p.1-5 |
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description | AC losses induced by magnetic field variations dissipate power in the conductors of coils during the tokamak operation. They can be critical for being a possible source of resistive transitions and leading to a possible quench in the magnet. This paper aims at presenting the results of the influence of the applied field direction on these losses. The measurements are carried out at the JOSEFA facility on one JT-60SA TF sample taken from the production length. In a tokamak environment, the field direction is perpendicular either to the conductor large side or small side. If the coupling losses in the cable are compared for the two field directions, it is evidenced that the losses are significantly larger when the field is transverse to the wide side. This is particularly true for the low frequencies. It will be shown in the following that, even for rather small aspect ratio, the losses are quite different for the two directions. In a second time, the measured coupling losses in the usual form of an Energy/cycle vs frequency curve, are fitted with the MPAS model to derive the parameters needed for any further calculations. In addition, a verifying test has been conducted by a comparison of direct measurements of trapezoidal field pulses in the JOSEFA facility, with the calculations made with the parameters issued from the fit with MPAS. |
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They can be critical for being a possible source of resistive transitions and leading to a possible quench in the magnet. This paper aims at presenting the results of the influence of the applied field direction on these losses. The measurements are carried out at the JOSEFA facility on one JT-60SA TF sample taken from the production length. In a tokamak environment, the field direction is perpendicular either to the conductor large side or small side. If the coupling losses in the cable are compared for the two field directions, it is evidenced that the losses are significantly larger when the field is transverse to the wide side. This is particularly true for the low frequencies. It will be shown in the following that, even for rather small aspect ratio, the losses are quite different for the two directions. In a second time, the measured coupling losses in the usual form of an Energy/cycle vs frequency curve, are fitted with the MPAS model to derive the parameters needed for any further calculations. In addition, a verifying test has been conducted by a comparison of direct measurements of trapezoidal field pulses in the JOSEFA facility, with the calculations made with the parameters issued from the fit with MPAS.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2024.3361437</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>AC loss ; Aspect ratio ; CICC ; Conductors ; Coupling ; Couplings ; Frequency measurement ; Length measurement ; Loss measurement ; Magnetic field measurement ; Mathematical models ; MPAS model ; Parameters ; superconducting magnets ; Superconductivity ; Tokamak devices ; X-ray tomography</subject><ispartof>IEEE transactions on applied superconductivity, 2024-08, Vol.34 (5), p.1-5</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2024</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c246t-8d24a5404e5c5b4abc8e078640fd7b3f91615f33fddcdcebcf7e2eda4e05f0343</cites><orcidid>0000-0002-3627-2521 ; 0000-0002-9079-7281 ; 0000-0001-7987-7179 ; 0000-0002-3653-0527 ; 0000-0002-5368-2995</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/10439060$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,777,781,793,27905,27906,54739</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/10439060$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Babouche, R.</creatorcontrib><creatorcontrib>Duchateau, J.-L.</creatorcontrib><creatorcontrib>Torre, A.</creatorcontrib><creatorcontrib>Topin, F.</creatorcontrib><creatorcontrib>Turck, B.</creatorcontrib><creatorcontrib>Zani, L.</creatorcontrib><title>Influence of Field Direction and Conductor Aspect Ratio on Coupling Losses: Measurements and Modeling on the JT-60SA TF Conductor</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>AC losses induced by magnetic field variations dissipate power in the conductors of coils during the tokamak operation. They can be critical for being a possible source of resistive transitions and leading to a possible quench in the magnet. This paper aims at presenting the results of the influence of the applied field direction on these losses. The measurements are carried out at the JOSEFA facility on one JT-60SA TF sample taken from the production length. In a tokamak environment, the field direction is perpendicular either to the conductor large side or small side. If the coupling losses in the cable are compared for the two field directions, it is evidenced that the losses are significantly larger when the field is transverse to the wide side. This is particularly true for the low frequencies. It will be shown in the following that, even for rather small aspect ratio, the losses are quite different for the two directions. In a second time, the measured coupling losses in the usual form of an Energy/cycle vs frequency curve, are fitted with the MPAS model to derive the parameters needed for any further calculations. In addition, a verifying test has been conducted by a comparison of direct measurements of trapezoidal field pulses in the JOSEFA facility, with the calculations made with the parameters issued from the fit with MPAS.</description><subject>AC loss</subject><subject>Aspect ratio</subject><subject>CICC</subject><subject>Conductors</subject><subject>Coupling</subject><subject>Couplings</subject><subject>Frequency measurement</subject><subject>Length measurement</subject><subject>Loss measurement</subject><subject>Magnetic field measurement</subject><subject>Mathematical models</subject><subject>MPAS model</subject><subject>Parameters</subject><subject>superconducting magnets</subject><subject>Superconductivity</subject><subject>Tokamak devices</subject><subject>X-ray tomography</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNpNkMtOwzAQRSMEEqXwAUgsLLFO8TMPdlGgUNQKiYZ1lNhjSJXGwU4WLPlz3IcEK488585oThBcEzwjBKd3RbbOZxRTPmMsIpzFJ8GECJGEVBBx6mssSJhQys6DC-c2GBOecDEJfhadbkfoJCCj0byBVqGHxoIcGtOhqlMoN50a5WAsylzv_9Fb5XvId3Mz9m3TfaClcQ7cPVpB5UYLW-gGt8-ujII94enhE9BLEUZ4naFi_jf2MjjTVevg6vhOg_f5Y5E_h8vXp0WeLUNJeTSEiaK8EhxzEFLUvKplAjhOIo61imumUxIRoRnTSkkloZY6Bgqq4oCFxoyzaXB7mNtb8zWCG8qNGW3nV5Y09dJwKtLEU-RASeuPsqDL3jbbyn6XBJc70-XOdLkzXR5N-8zNIdMAwD-esxRHmP0CyvJ6ww</recordid><startdate>20240801</startdate><enddate>20240801</enddate><creator>Babouche, R.</creator><creator>Duchateau, J.-L.</creator><creator>Torre, A.</creator><creator>Topin, F.</creator><creator>Turck, B.</creator><creator>Zani, L.</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><orcidid>https://orcid.org/0000-0002-3627-2521</orcidid><orcidid>https://orcid.org/0000-0002-9079-7281</orcidid><orcidid>https://orcid.org/0000-0001-7987-7179</orcidid><orcidid>https://orcid.org/0000-0002-3653-0527</orcidid><orcidid>https://orcid.org/0000-0002-5368-2995</orcidid></search><sort><creationdate>20240801</creationdate><title>Influence of Field Direction and Conductor Aspect Ratio on Coupling Losses: Measurements and Modeling on the JT-60SA TF Conductor</title><author>Babouche, R. ; Duchateau, J.-L. ; Torre, A. ; Topin, F. ; Turck, B. ; Zani, L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c246t-8d24a5404e5c5b4abc8e078640fd7b3f91615f33fddcdcebcf7e2eda4e05f0343</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>AC loss</topic><topic>Aspect ratio</topic><topic>CICC</topic><topic>Conductors</topic><topic>Coupling</topic><topic>Couplings</topic><topic>Frequency measurement</topic><topic>Length measurement</topic><topic>Loss measurement</topic><topic>Magnetic field measurement</topic><topic>Mathematical models</topic><topic>MPAS model</topic><topic>Parameters</topic><topic>superconducting magnets</topic><topic>Superconductivity</topic><topic>Tokamak devices</topic><topic>X-ray tomography</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Babouche, R.</creatorcontrib><creatorcontrib>Duchateau, J.-L.</creatorcontrib><creatorcontrib>Torre, A.</creatorcontrib><creatorcontrib>Topin, F.</creatorcontrib><creatorcontrib>Turck, B.</creatorcontrib><creatorcontrib>Zani, L.</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>Babouche, R.</au><au>Duchateau, J.-L.</au><au>Torre, A.</au><au>Topin, F.</au><au>Turck, B.</au><au>Zani, L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Influence of Field Direction and Conductor Aspect Ratio on Coupling Losses: Measurements and Modeling on the JT-60SA TF Conductor</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><stitle>TASC</stitle><date>2024-08-01</date><risdate>2024</risdate><volume>34</volume><issue>5</issue><spage>1</spage><epage>5</epage><pages>1-5</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><coden>ITASE9</coden><abstract>AC losses induced by magnetic field variations dissipate power in the conductors of coils during the tokamak operation. They can be critical for being a possible source of resistive transitions and leading to a possible quench in the magnet. This paper aims at presenting the results of the influence of the applied field direction on these losses. The measurements are carried out at the JOSEFA facility on one JT-60SA TF sample taken from the production length. In a tokamak environment, the field direction is perpendicular either to the conductor large side or small side. If the coupling losses in the cable are compared for the two field directions, it is evidenced that the losses are significantly larger when the field is transverse to the wide side. This is particularly true for the low frequencies. It will be shown in the following that, even for rather small aspect ratio, the losses are quite different for the two directions. In a second time, the measured coupling losses in the usual form of an Energy/cycle vs frequency curve, are fitted with the MPAS model to derive the parameters needed for any further calculations. In addition, a verifying test has been conducted by a comparison of direct measurements of trapezoidal field pulses in the JOSEFA facility, with the calculations made with the parameters issued from the fit with MPAS.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TASC.2024.3361437</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0002-3627-2521</orcidid><orcidid>https://orcid.org/0000-0002-9079-7281</orcidid><orcidid>https://orcid.org/0000-0001-7987-7179</orcidid><orcidid>https://orcid.org/0000-0002-3653-0527</orcidid><orcidid>https://orcid.org/0000-0002-5368-2995</orcidid></addata></record> |
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subjects | AC loss Aspect ratio CICC Conductors Coupling Couplings Frequency measurement Length measurement Loss measurement Magnetic field measurement Mathematical models MPAS model Parameters superconducting magnets Superconductivity Tokamak devices X-ray tomography |
title | Influence of Field Direction and Conductor Aspect Ratio on Coupling Losses: Measurements and Modeling on the JT-60SA TF Conductor |
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