CURRENT LEAD FOR HIGH-TEMPERATURE SUPERCONDUCTING (HTS) CABLE AND DESIGN METHOD THEREOF
The present disclosure provides a current lead structure for a high-temperature superconducting (HTS) cable and a design method thereof. The current lead structure includes a plurality of metal rods arranged in parallel at a preset interval along an axial direction of a current lead, where the metal...
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creator | ZHANG, Xize HUANG, Yijia YANG, Jianping ZHENG, Jian WEI, Bengang ZONG, Xihua ZHANG, Zhiyong CHEN, Zhiyue JIAO, Ting ZHANG, Qiqi HAN, Yunwu LI, Honglei |
description | The present disclosure provides a current lead structure for a high-temperature superconducting (HTS) cable and a design method thereof. The current lead structure includes a plurality of metal rods arranged in parallel at a preset interval along an axial direction of a current lead, where the metal rod includes a first lead segment, a second lead segment, and a third lead segment; a bottom end of the first lead segment is in contact with a liquid nitrogen level, and a top end of the first lead segment is connected to a bottom end of the second lead segment; a top end of the second lead segment is connected to a bottom end of the third lead segment, and a top end of the third lead segment is connected to a room-temperature wiring terminal; the first lead segment and the third lead segment are solid metal rods, and the second lead segment is a hollow metal rod; and the top end of the second lead segment is not higher than a position of an epoxy board. A hollow groove is formed inside to form a simple structure, which significantly optimizes a thermal field distribution, reduces a heat leakage of the current lead, and provides a reliable support for the subsequent design of the current lead. A current lead with the structure is easy to manufacture, install, and maintain, which is conducive to engineering promotion and application. Step 1: measure a distance between the liquid nitrogen level in a terminal of the HTS cable and the room-temperature wiring terminal, and a distance between the liquid nitrogen level and the epoxy board; and determine lengths of the first lead segment, the second lead segment, and the third lead segment ofthe current lead separately Step 2: measure an outer diameter of the current lead, and set an initial value of an inner diameter ofthe second lead segment of the current lead based on a rated current ofthe current lead Step 3: measure a temperature of the liquid nitrogen level, a temperature of the position of the epoxy board, and a temperature of the room-temperature wiring terminal Step 4: based on a coupling model of a thermal field and an electric field ofthe current lead, and with a minimum heat leakage ofthe current lead as an objective function, use a simulation method to optimize the length and the inner diameter of the second lead segment starting from the initial value of the inner diameter of the second lead segment Step 5: re-determine the lengths of the first lead segment and the third lead segment of the current lead |
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The current lead structure includes a plurality of metal rods arranged in parallel at a preset interval along an axial direction of a current lead, where the metal rod includes a first lead segment, a second lead segment, and a third lead segment; a bottom end of the first lead segment is in contact with a liquid nitrogen level, and a top end of the first lead segment is connected to a bottom end of the second lead segment; a top end of the second lead segment is connected to a bottom end of the third lead segment, and a top end of the third lead segment is connected to a room-temperature wiring terminal; the first lead segment and the third lead segment are solid metal rods, and the second lead segment is a hollow metal rod; and the top end of the second lead segment is not higher than a position of an epoxy board. A hollow groove is formed inside to form a simple structure, which significantly optimizes a thermal field distribution, reduces a heat leakage of the current lead, and provides a reliable support for the subsequent design of the current lead. A current lead with the structure is easy to manufacture, install, and maintain, which is conducive to engineering promotion and application. Step 1: measure a distance between the liquid nitrogen level in a terminal of the HTS cable and the room-temperature wiring terminal, and a distance between the liquid nitrogen level and the epoxy board; and determine lengths of the first lead segment, the second lead segment, and the third lead segment ofthe current lead separately Step 2: measure an outer diameter of the current lead, and set an initial value of an inner diameter ofthe second lead segment of the current lead based on a rated current ofthe current lead Step 3: measure a temperature of the liquid nitrogen level, a temperature of the position of the epoxy board, and a temperature of the room-temperature wiring terminal Step 4: based on a coupling model of a thermal field and an electric field ofthe current lead, and with a minimum heat leakage ofthe current lead as an objective function, use a simulation method to optimize the length and the inner diameter of the second lead segment starting from the initial value of the inner diameter of the second lead segment Step 5: re-determine the lengths of the first lead segment and the third lead segment of the current lead based on optimization results of the length and the inner diameter of the second lead segment</description><language>eng</language><subject>BASIC ELECTRIC ELEMENTS ; CABLES ; CONDUCTORS ; ELECTRICITY ; INSULATORS ; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING ORDIELECTRIC PROPERTIES</subject><creationdate>2023</creationdate><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://worldwide.espacenet.com/publicationDetails/biblio?FT=D&date=20230831&DB=EPODOC&CC=AU&NR=2021355610B2$$EHTML$$P50$$Gepo$$Hfree_for_read</linktohtml><link.rule.ids>230,308,776,881,25542,76289</link.rule.ids><linktorsrc>$$Uhttps://worldwide.espacenet.com/publicationDetails/biblio?FT=D&date=20230831&DB=EPODOC&CC=AU&NR=2021355610B2$$EView_record_in_European_Patent_Office$$FView_record_in_$$GEuropean_Patent_Office$$Hfree_for_read</linktorsrc></links><search><creatorcontrib>ZHANG, Xize</creatorcontrib><creatorcontrib>HUANG, Yijia</creatorcontrib><creatorcontrib>YANG, Jianping</creatorcontrib><creatorcontrib>ZHENG, Jian</creatorcontrib><creatorcontrib>WEI, Bengang</creatorcontrib><creatorcontrib>ZONG, Xihua</creatorcontrib><creatorcontrib>ZHANG, Zhiyong</creatorcontrib><creatorcontrib>CHEN, Zhiyue</creatorcontrib><creatorcontrib>JIAO, Ting</creatorcontrib><creatorcontrib>ZHANG, Qiqi</creatorcontrib><creatorcontrib>HAN, Yunwu</creatorcontrib><creatorcontrib>LI, Honglei</creatorcontrib><title>CURRENT LEAD FOR HIGH-TEMPERATURE SUPERCONDUCTING (HTS) CABLE AND DESIGN METHOD THEREOF</title><description>The present disclosure provides a current lead structure for a high-temperature superconducting (HTS) cable and a design method thereof. The current lead structure includes a plurality of metal rods arranged in parallel at a preset interval along an axial direction of a current lead, where the metal rod includes a first lead segment, a second lead segment, and a third lead segment; a bottom end of the first lead segment is in contact with a liquid nitrogen level, and a top end of the first lead segment is connected to a bottom end of the second lead segment; a top end of the second lead segment is connected to a bottom end of the third lead segment, and a top end of the third lead segment is connected to a room-temperature wiring terminal; the first lead segment and the third lead segment are solid metal rods, and the second lead segment is a hollow metal rod; and the top end of the second lead segment is not higher than a position of an epoxy board. A hollow groove is formed inside to form a simple structure, which significantly optimizes a thermal field distribution, reduces a heat leakage of the current lead, and provides a reliable support for the subsequent design of the current lead. A current lead with the structure is easy to manufacture, install, and maintain, which is conducive to engineering promotion and application. Step 1: measure a distance between the liquid nitrogen level in a terminal of the HTS cable and the room-temperature wiring terminal, and a distance between the liquid nitrogen level and the epoxy board; and determine lengths of the first lead segment, the second lead segment, and the third lead segment ofthe current lead separately Step 2: measure an outer diameter of the current lead, and set an initial value of an inner diameter ofthe second lead segment of the current lead based on a rated current ofthe current lead Step 3: measure a temperature of the liquid nitrogen level, a temperature of the position of the epoxy board, and a temperature of the room-temperature wiring terminal Step 4: based on a coupling model of a thermal field and an electric field ofthe current lead, and with a minimum heat leakage ofthe current lead as an objective function, use a simulation method to optimize the length and the inner diameter of the second lead segment starting from the initial value of the inner diameter of the second lead segment Step 5: re-determine the lengths of the first lead segment and the third lead segment of the current lead based on optimization results of the length and the inner diameter of the second lead segment</description><subject>BASIC ELECTRIC ELEMENTS</subject><subject>CABLES</subject><subject>CONDUCTORS</subject><subject>ELECTRICITY</subject><subject>INSULATORS</subject><subject>SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING ORDIELECTRIC PROPERTIES</subject><fulltext>true</fulltext><rsrctype>patent</rsrctype><creationdate>2023</creationdate><recordtype>patent</recordtype><sourceid>EVB</sourceid><recordid>eNqNyr0KwjAUQOEuDqK-wx0cdCi0Ke2eJjc_0CaS3OBYisRJtFDfHx18AKfzDWdbXEUKAR3BgFyC8gGM1aYkHC8YOKWAENOXwjuZBFmn4WQonkHwfkDgToLEaLWDEcl4CWQwoFf7YnOfH2s-_LorjgpJmDIvrymvy3zLz_yeeGIVq5u27eqq71nz5_YBwzsx9A</recordid><startdate>20230831</startdate><enddate>20230831</enddate><creator>ZHANG, Xize</creator><creator>HUANG, Yijia</creator><creator>YANG, Jianping</creator><creator>ZHENG, Jian</creator><creator>WEI, Bengang</creator><creator>ZONG, Xihua</creator><creator>ZHANG, Zhiyong</creator><creator>CHEN, Zhiyue</creator><creator>JIAO, Ting</creator><creator>ZHANG, Qiqi</creator><creator>HAN, Yunwu</creator><creator>LI, Honglei</creator><scope>EVB</scope></search><sort><creationdate>20230831</creationdate><title>CURRENT LEAD FOR HIGH-TEMPERATURE SUPERCONDUCTING (HTS) CABLE AND DESIGN METHOD THEREOF</title><author>ZHANG, Xize ; HUANG, Yijia ; YANG, Jianping ; ZHENG, Jian ; WEI, Bengang ; ZONG, Xihua ; ZHANG, Zhiyong ; CHEN, Zhiyue ; JIAO, Ting ; ZHANG, Qiqi ; HAN, Yunwu ; LI, Honglei</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-epo_espacenet_AU2021355610BB23</frbrgroupid><rsrctype>patents</rsrctype><prefilter>patents</prefilter><language>eng</language><creationdate>2023</creationdate><topic>BASIC ELECTRIC ELEMENTS</topic><topic>CABLES</topic><topic>CONDUCTORS</topic><topic>ELECTRICITY</topic><topic>INSULATORS</topic><topic>SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING ORDIELECTRIC PROPERTIES</topic><toplevel>online_resources</toplevel><creatorcontrib>ZHANG, Xize</creatorcontrib><creatorcontrib>HUANG, Yijia</creatorcontrib><creatorcontrib>YANG, Jianping</creatorcontrib><creatorcontrib>ZHENG, Jian</creatorcontrib><creatorcontrib>WEI, Bengang</creatorcontrib><creatorcontrib>ZONG, Xihua</creatorcontrib><creatorcontrib>ZHANG, Zhiyong</creatorcontrib><creatorcontrib>CHEN, Zhiyue</creatorcontrib><creatorcontrib>JIAO, Ting</creatorcontrib><creatorcontrib>ZHANG, Qiqi</creatorcontrib><creatorcontrib>HAN, Yunwu</creatorcontrib><creatorcontrib>LI, Honglei</creatorcontrib><collection>esp@cenet</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>ZHANG, Xize</au><au>HUANG, Yijia</au><au>YANG, Jianping</au><au>ZHENG, Jian</au><au>WEI, Bengang</au><au>ZONG, Xihua</au><au>ZHANG, Zhiyong</au><au>CHEN, Zhiyue</au><au>JIAO, Ting</au><au>ZHANG, Qiqi</au><au>HAN, Yunwu</au><au>LI, Honglei</au><format>patent</format><genre>patent</genre><ristype>GEN</ristype><title>CURRENT LEAD FOR HIGH-TEMPERATURE SUPERCONDUCTING (HTS) CABLE AND DESIGN METHOD THEREOF</title><date>2023-08-31</date><risdate>2023</risdate><abstract>The present disclosure provides a current lead structure for a high-temperature superconducting (HTS) cable and a design method thereof. The current lead structure includes a plurality of metal rods arranged in parallel at a preset interval along an axial direction of a current lead, where the metal rod includes a first lead segment, a second lead segment, and a third lead segment; a bottom end of the first lead segment is in contact with a liquid nitrogen level, and a top end of the first lead segment is connected to a bottom end of the second lead segment; a top end of the second lead segment is connected to a bottom end of the third lead segment, and a top end of the third lead segment is connected to a room-temperature wiring terminal; the first lead segment and the third lead segment are solid metal rods, and the second lead segment is a hollow metal rod; and the top end of the second lead segment is not higher than a position of an epoxy board. A hollow groove is formed inside to form a simple structure, which significantly optimizes a thermal field distribution, reduces a heat leakage of the current lead, and provides a reliable support for the subsequent design of the current lead. A current lead with the structure is easy to manufacture, install, and maintain, which is conducive to engineering promotion and application. Step 1: measure a distance between the liquid nitrogen level in a terminal of the HTS cable and the room-temperature wiring terminal, and a distance between the liquid nitrogen level and the epoxy board; and determine lengths of the first lead segment, the second lead segment, and the third lead segment ofthe current lead separately Step 2: measure an outer diameter of the current lead, and set an initial value of an inner diameter ofthe second lead segment of the current lead based on a rated current ofthe current lead Step 3: measure a temperature of the liquid nitrogen level, a temperature of the position of the epoxy board, and a temperature of the room-temperature wiring terminal Step 4: based on a coupling model of a thermal field and an electric field ofthe current lead, and with a minimum heat leakage ofthe current lead as an objective function, use a simulation method to optimize the length and the inner diameter of the second lead segment starting from the initial value of the inner diameter of the second lead segment Step 5: re-determine the lengths of the first lead segment and the third lead segment of the current lead based on optimization results of the length and the inner diameter of the second lead segment</abstract><oa>free_for_read</oa></addata></record> |
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subjects | BASIC ELECTRIC ELEMENTS CABLES CONDUCTORS ELECTRICITY INSULATORS SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING ORDIELECTRIC PROPERTIES |
title | CURRENT LEAD FOR HIGH-TEMPERATURE SUPERCONDUCTING (HTS) CABLE AND DESIGN METHOD THEREOF |
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