Stray Field of SMES Coil Configurations
A stray field from a superconducting coil restricts the use of SMES at a demand site, though SMES has an attractive potential for power management and quality control. The stray field outside a solenoid is analyzed by a series of Legendre polynomials, and the results are then applied to various coil...
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Veröffentlicht in: | TEION KOGAKU (Journal of Cryogenics and Superconductivity Society of Japan) 1998/12/25, Vol.33(12), pp.773-781 |
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container_title | TEION KOGAKU (Journal of Cryogenics and Superconductivity Society of Japan) |
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creator | HAMAJIMA, Takataro SHIMADA, Mamoru HANAI, Satoshi WACHI, Yoshihiro TEZUKA, Masaru TAKANO, Hirohisa |
description | A stray field from a superconducting coil restricts the use of SMES at a demand site, though SMES has an attractive potential for power management and quality control. The stray field outside a solenoid is analyzed by a series of Legendre polynomials, and the results are then applied to various coil configurations. The summation of magnetic moments from all coils must be zero, which leads the stray field decreasing as Rp-3 to vanish, where Rp is distance from the coil. The higher order of the stray field can be cancelled out if the coil arrangement is optimized. In this paper, we treat a single solenoid as a reference, and active shield coil, axially displaced coil, multipole coil and toroidal coil configurations to reduce the stray field. It is shown that the stray field from the active shield coil configuration decreases as Rp-7. On the other hand, the stray field from an axially displaced coil drops as a function of Rp-5. The multipole coil configuration has high potential to reduce the stray field because the stray field behaves like Rp-(n/2+3), where n is the coil number. The toroidal coil configuration has the stray field decreasing as Rp-(n+2), though it has alarge volume facility. |
doi_str_mv | 10.2221/jcsj.33.773 |
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The stray field outside a solenoid is analyzed by a series of Legendre polynomials, and the results are then applied to various coil configurations. The summation of magnetic moments from all coils must be zero, which leads the stray field decreasing as Rp-3 to vanish, where Rp is distance from the coil. The higher order of the stray field can be cancelled out if the coil arrangement is optimized. In this paper, we treat a single solenoid as a reference, and active shield coil, axially displaced coil, multipole coil and toroidal coil configurations to reduce the stray field. It is shown that the stray field from the active shield coil configuration decreases as Rp-7. On the other hand, the stray field from an axially displaced coil drops as a function of Rp-5. The multipole coil configuration has high potential to reduce the stray field because the stray field behaves like Rp-(n/2+3), where n is the coil number. 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The toroidal coil configuration has the stray field decreasing as Rp-(n+2), though it has alarge volume facility.</description><subject>Legendre polynomials</subject><subject>magnetic moment</subject><subject>SMES</subject><subject>solenoid coil</subject><subject>stray field</subject><issn>0389-2441</issn><issn>1880-0408</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1998</creationdate><recordtype>article</recordtype><recordid>eNo9zzFPwzAQBWALgUQpTPyBbAwo4c7nJM6IorYgFTEEZstx7JIoNMgOQ_89Ca26vFu-d9Jj7B4h4ZzjU2dClxAleU4XbIFSQgwC5CVbAMki5kLgNbsJoQMQmGK2YA_V6PUhWre2b6LBRdXbqorKoe2n2Lt29-v12A77cMuunO6DvTvdJftcrz7Kl3j7vnktn7ex4ZRSTKJxwjaGp4JzS7KWBinNm1rbzEoDhcyFI2wcWO5qw2sCxAJSB5mTtiloyR6Pf40fQvDWqR_ffmt_UAhq3qjmjYpITRsnvT7qLox6Z89W-7E1vf23WGTZ7JGfciqegfnSXtk9_QGck1wl</recordid><startdate>1998</startdate><enddate>1998</enddate><creator>HAMAJIMA, Takataro</creator><creator>SHIMADA, Mamoru</creator><creator>HANAI, Satoshi</creator><creator>WACHI, Yoshihiro</creator><creator>TEZUKA, Masaru</creator><creator>TAKANO, Hirohisa</creator><general>CRYOGENICS AND SUPERCONDUCTIVITY SOCIETY OF JAPAN</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>1998</creationdate><title>Stray Field of SMES Coil Configurations</title><author>HAMAJIMA, Takataro ; SHIMADA, Mamoru ; HANAI, Satoshi ; WACHI, Yoshihiro ; TEZUKA, Masaru ; TAKANO, Hirohisa</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2353-34df4edc25422e38b8c1357dbae6e8c09874f31df0e2fbc2b3011905f06f8ed93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1998</creationdate><topic>Legendre polynomials</topic><topic>magnetic moment</topic><topic>SMES</topic><topic>solenoid coil</topic><topic>stray field</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>HAMAJIMA, Takataro</creatorcontrib><creatorcontrib>SHIMADA, Mamoru</creatorcontrib><creatorcontrib>HANAI, Satoshi</creatorcontrib><creatorcontrib>WACHI, Yoshihiro</creatorcontrib><creatorcontrib>TEZUKA, Masaru</creatorcontrib><creatorcontrib>TAKANO, Hirohisa</creatorcontrib><collection>CrossRef</collection><jtitle>TEION KOGAKU (Journal of Cryogenics and Superconductivity Society of Japan)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>HAMAJIMA, Takataro</au><au>SHIMADA, Mamoru</au><au>HANAI, Satoshi</au><au>WACHI, Yoshihiro</au><au>TEZUKA, Masaru</au><au>TAKANO, Hirohisa</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Stray Field of SMES Coil Configurations</atitle><jtitle>TEION KOGAKU (Journal of Cryogenics and Superconductivity Society of Japan)</jtitle><addtitle>TEION KOGAKU</addtitle><date>1998</date><risdate>1998</risdate><volume>33</volume><issue>12</issue><spage>773</spage><epage>781</epage><pages>773-781</pages><issn>0389-2441</issn><eissn>1880-0408</eissn><abstract>A stray field from a superconducting coil restricts the use of SMES at a demand site, though SMES has an attractive potential for power management and quality control. The stray field outside a solenoid is analyzed by a series of Legendre polynomials, and the results are then applied to various coil configurations. The summation of magnetic moments from all coils must be zero, which leads the stray field decreasing as Rp-3 to vanish, where Rp is distance from the coil. The higher order of the stray field can be cancelled out if the coil arrangement is optimized. In this paper, we treat a single solenoid as a reference, and active shield coil, axially displaced coil, multipole coil and toroidal coil configurations to reduce the stray field. It is shown that the stray field from the active shield coil configuration decreases as Rp-7. On the other hand, the stray field from an axially displaced coil drops as a function of Rp-5. The multipole coil configuration has high potential to reduce the stray field because the stray field behaves like Rp-(n/2+3), where n is the coil number. The toroidal coil configuration has the stray field decreasing as Rp-(n+2), though it has alarge volume facility.</abstract><pub>CRYOGENICS AND SUPERCONDUCTIVITY SOCIETY OF JAPAN</pub><doi>10.2221/jcsj.33.773</doi><tpages>9</tpages><oa>free_for_read</oa></addata></record> |
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language | eng |
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source | Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals |
subjects | Legendre polynomials magnetic moment SMES solenoid coil stray field |
title | Stray Field of SMES Coil Configurations |
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