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Effect of Bubbles on Liquid Nitrogen Breakdown in Plane-Plane Electrode Geometry From 100-250 kPa
Liquid nitrogen (LN 2 ) is used as the cryogen and dielectric for many high temperature superconducting, high voltage applications. When a quench in the superconductor occurs, bubbles are generated which can affect the dielectric breakdown properties of the LN 2 . Experiments were performed using pl...
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Published in: | IEEE transactions on applied superconductivity 2011-06, Vol.21 (3), p.1892-1895 |
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description | Liquid nitrogen (LN 2 ) is used as the cryogen and dielectric for many high temperature superconducting, high voltage applications. When a quench in the superconductor occurs, bubbles are generated which can affect the dielectric breakdown properties of the LN 2 . Experiments were performed using plane-plane electrode geometry where bubbles were introduced into the gap through a pinhole in the ground electrode. Bubbles were generated using one or more kapton heaters producing heater powers up to 30 W. Pressure was varied from 100-250 kPa. Breakdown strength was found to be relatively constant up to a given heater power and pressure at which the breakdown strength drops to a low value depending on the pressure. After the drop the breakdown strength continues to drop gradually at higher heater power. This is particularly illustrated at 100 kPa. After the drop in breakdown strength the breakdown is believed to be due to the formation of a vapor bridge. Also the heater power at which the breakdown strength changes from that of LN 2 to that of gaseous nitrogen increases with increasing pressure. The data can provide design constraints for high temperature superconducting fault current limiters (FCLs) so that the formation of a vapor bridge can be suppressed or avoided. |
doi_str_mv | 10.1109/TASC.2010.2088351 |
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(ORNL), Oak Ridge, TN (United States)</creatorcontrib><description>Liquid nitrogen (LN 2 ) is used as the cryogen and dielectric for many high temperature superconducting, high voltage applications. When a quench in the superconductor occurs, bubbles are generated which can affect the dielectric breakdown properties of the LN 2 . Experiments were performed using plane-plane electrode geometry where bubbles were introduced into the gap through a pinhole in the ground electrode. Bubbles were generated using one or more kapton heaters producing heater powers up to 30 W. Pressure was varied from 100-250 kPa. Breakdown strength was found to be relatively constant up to a given heater power and pressure at which the breakdown strength drops to a low value depending on the pressure. After the drop the breakdown strength continues to drop gradually at higher heater power. This is particularly illustrated at 100 kPa. After the drop in breakdown strength the breakdown is believed to be due to the formation of a vapor bridge. Also the heater power at which the breakdown strength changes from that of LN 2 to that of gaseous nitrogen increases with increasing pressure. The data can provide design constraints for high temperature superconducting fault current limiters (FCLs) so that the formation of a vapor bridge can be suppressed or avoided.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2010.2088351</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; BREAKDOWN ; Bridge circuits ; BUBBLES ; CRYOGENIC FLUIDS ; CURRENT LIMITERS ; DESIGN ; DIELECTRIC MATERIALS ; Electric breakdown ; Electric power plants ; Electrical engineering. Electrical power engineering ; Electrical power engineering ; ELECTRODES ; Electromagnets ; Electronics ; Exact sciences and technology ; FCL ; GEOMETRY ; HEATERS ; Heating ; High temperature ; High temperature superconductors ; MATERIALS SCIENCE ; Miscellaneous ; NITROGEN ; quench ; Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices ; Superconducting devices ; SUPERCONDUCTORS ; Various equipment and components ; {\rm LN}_{2}</subject><ispartof>IEEE transactions on applied superconductivity, 2011-06, Vol.21 (3), p.1892-1895</ispartof><rights>2015 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) Jun 2011</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c349t-2107424d7a1c423c37a5d3c909b5fb59f1df3dc3961b496b0305355dc0ad8e063</citedby><cites>FETCH-LOGICAL-c349t-2107424d7a1c423c37a5d3c909b5fb59f1df3dc3961b496b0305355dc0ad8e063</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/5639052$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>230,309,310,314,776,780,785,786,881,23909,23910,25118,27901,27902,54771</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=24274518$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/1036583$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Sauers, I</creatorcontrib><creatorcontrib>James, R</creatorcontrib><creatorcontrib>Ellis, A</creatorcontrib><creatorcontrib>Tuncer, E</creatorcontrib><creatorcontrib>Polizos, G</creatorcontrib><creatorcontrib>Pace, M</creatorcontrib><creatorcontrib>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</creatorcontrib><title>Effect of Bubbles on Liquid Nitrogen Breakdown in Plane-Plane Electrode Geometry From 100-250 kPa</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>Liquid nitrogen (LN 2 ) is used as the cryogen and dielectric for many high temperature superconducting, high voltage applications. When a quench in the superconductor occurs, bubbles are generated which can affect the dielectric breakdown properties of the LN 2 . Experiments were performed using plane-plane electrode geometry where bubbles were introduced into the gap through a pinhole in the ground electrode. Bubbles were generated using one or more kapton heaters producing heater powers up to 30 W. Pressure was varied from 100-250 kPa. Breakdown strength was found to be relatively constant up to a given heater power and pressure at which the breakdown strength drops to a low value depending on the pressure. After the drop the breakdown strength continues to drop gradually at higher heater power. This is particularly illustrated at 100 kPa. After the drop in breakdown strength the breakdown is believed to be due to the formation of a vapor bridge. Also the heater power at which the breakdown strength changes from that of LN 2 to that of gaseous nitrogen increases with increasing pressure. The data can provide design constraints for high temperature superconducting fault current limiters (FCLs) so that the formation of a vapor bridge can be suppressed or avoided.</description><subject>Applied sciences</subject><subject>BREAKDOWN</subject><subject>Bridge circuits</subject><subject>BUBBLES</subject><subject>CRYOGENIC FLUIDS</subject><subject>CURRENT LIMITERS</subject><subject>DESIGN</subject><subject>DIELECTRIC MATERIALS</subject><subject>Electric breakdown</subject><subject>Electric power plants</subject><subject>Electrical engineering. Electrical power engineering</subject><subject>Electrical power engineering</subject><subject>ELECTRODES</subject><subject>Electromagnets</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>FCL</subject><subject>GEOMETRY</subject><subject>HEATERS</subject><subject>Heating</subject><subject>High temperature</subject><subject>High temperature superconductors</subject><subject>MATERIALS SCIENCE</subject><subject>Miscellaneous</subject><subject>NITROGEN</subject><subject>quench</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</subject><subject>Superconducting devices</subject><subject>SUPERCONDUCTORS</subject><subject>Various equipment and components</subject><subject>{\rm LN}_{2}</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNpFkN1rFDEUxQdRsFb_APElCD5Ovfm4M8lju2xrYdGC9Tlk8qFpZ5M2mUX635t1l_YlySW_c-7hdN1HCmeUgvp6e_5zdcagjQyk5EhfdScUUfYMKb5ub0DaS8b42-5drXcAVEiBJ51Zh-DtQnIgF7tpmn0lOZFNfNxFR77HpeTfPpGL4s29y38TiYnczCb5_v9J1nMTl-w8ufJ565fyRC5L3hIK0DYDub8x77s3wczVfzjep92vy_Xt6lu_-XF1vTrf9JYLtfSMwiiYcKOhVjBu-WjQcatATRgmVIG6wJ3laqCTUMMEHJAjOgvGSQ8DP-0-H3xzXaKuNi7e_rE5pZZQU-ADSv4CPZT8uPN10Xd5V1LLpRXFQfJxZA2iB8iWXGvxQT-UuDXlqdnofdt637bet62PbTfNl6OxqdbMoZhkY30WMsFGgVQ27tOBi977528cuAJk_B_4SIS4</recordid><startdate>20110601</startdate><enddate>20110601</enddate><creator>Sauers, I</creator><creator>James, R</creator><creator>Ellis, A</creator><creator>Tuncer, E</creator><creator>Polizos, G</creator><creator>Pace, M</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>OTOTI</scope></search><sort><creationdate>20110601</creationdate><title>Effect of Bubbles on Liquid Nitrogen Breakdown in Plane-Plane Electrode Geometry From 100-250 kPa</title><author>Sauers, I ; James, R ; Ellis, A ; Tuncer, E ; Polizos, G ; Pace, M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c349t-2107424d7a1c423c37a5d3c909b5fb59f1df3dc3961b496b0305355dc0ad8e063</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Applied sciences</topic><topic>BREAKDOWN</topic><topic>Bridge circuits</topic><topic>BUBBLES</topic><topic>CRYOGENIC FLUIDS</topic><topic>CURRENT LIMITERS</topic><topic>DESIGN</topic><topic>DIELECTRIC MATERIALS</topic><topic>Electric breakdown</topic><topic>Electric power plants</topic><topic>Electrical engineering. Electrical power engineering</topic><topic>Electrical power engineering</topic><topic>ELECTRODES</topic><topic>Electromagnets</topic><topic>Electronics</topic><topic>Exact sciences and technology</topic><topic>FCL</topic><topic>GEOMETRY</topic><topic>HEATERS</topic><topic>Heating</topic><topic>High temperature</topic><topic>High temperature superconductors</topic><topic>MATERIALS SCIENCE</topic><topic>Miscellaneous</topic><topic>NITROGEN</topic><topic>quench</topic><topic>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</topic><topic>Superconducting devices</topic><topic>SUPERCONDUCTORS</topic><topic>Various equipment and components</topic><topic>{\rm LN}_{2}</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sauers, I</creatorcontrib><creatorcontrib>James, R</creatorcontrib><creatorcontrib>Ellis, A</creatorcontrib><creatorcontrib>Tuncer, E</creatorcontrib><creatorcontrib>Polizos, G</creatorcontrib><creatorcontrib>Pace, M</creatorcontrib><creatorcontrib>Oak Ridge National Lab. 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(ORNL), Oak Ridge, TN (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of Bubbles on Liquid Nitrogen Breakdown in Plane-Plane Electrode Geometry From 100-250 kPa</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><stitle>TASC</stitle><date>2011-06-01</date><risdate>2011</risdate><volume>21</volume><issue>3</issue><spage>1892</spage><epage>1895</epage><pages>1892-1895</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><coden>ITASE9</coden><abstract>Liquid nitrogen (LN 2 ) is used as the cryogen and dielectric for many high temperature superconducting, high voltage applications. When a quench in the superconductor occurs, bubbles are generated which can affect the dielectric breakdown properties of the LN 2 . Experiments were performed using plane-plane electrode geometry where bubbles were introduced into the gap through a pinhole in the ground electrode. Bubbles were generated using one or more kapton heaters producing heater powers up to 30 W. Pressure was varied from 100-250 kPa. Breakdown strength was found to be relatively constant up to a given heater power and pressure at which the breakdown strength drops to a low value depending on the pressure. After the drop the breakdown strength continues to drop gradually at higher heater power. This is particularly illustrated at 100 kPa. After the drop in breakdown strength the breakdown is believed to be due to the formation of a vapor bridge. Also the heater power at which the breakdown strength changes from that of LN 2 to that of gaseous nitrogen increases with increasing pressure. The data can provide design constraints for high temperature superconducting fault current limiters (FCLs) so that the formation of a vapor bridge can be suppressed or avoided.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TASC.2010.2088351</doi><tpages>4</tpages></addata></record> |
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subjects | Applied sciences BREAKDOWN Bridge circuits BUBBLES CRYOGENIC FLUIDS CURRENT LIMITERS DESIGN DIELECTRIC MATERIALS Electric breakdown Electric power plants Electrical engineering. Electrical power engineering Electrical power engineering ELECTRODES Electromagnets Electronics Exact sciences and technology FCL GEOMETRY HEATERS Heating High temperature High temperature superconductors MATERIALS SCIENCE Miscellaneous NITROGEN quench Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices Superconducting devices SUPERCONDUCTORS Various equipment and components {\rm LN}_{2} |
title | Effect of Bubbles on Liquid Nitrogen Breakdown in Plane-Plane Electrode Geometry From 100-250 kPa |
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