The time and space characteristics of magnetomotive force in the cascaded linear induction motor
To choose a reasonable mode of three-phase winding for the improvement of the operating efficiency of cascaded linear induction motor, the time and space characteristics of magnetomotive force were investigated. The ideal model of the cascaded linear induction motor was built, in which the B and C-p...
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Veröffentlicht in: | Journal of modern transportation 2013-09, Vol.21 (3), p.194-199 |
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description | To choose a reasonable mode of three-phase winding for the improvement of the operating efficiency of cascaded linear induction motor, the time and space characteristics of magnetomotive force were investigated. The ideal model of the cascaded linear induction motor was built, in which the B and C-phase windings are respectively separated from the A-phase winding by a distance of d and e slots pitch and not overlapped. By changing the values of d and e from 1 to 5, we can obtain 20 different modes of three-phase winding with the different combinations of d and e. Then, the air-gap magnetomotive forces of A-, B-, and C-phase windings were calculated by the magnetomotive force theory. According to the transient superposition of magnetomotive forces of A-, B-, and C-phase windings, the theoretical and simulated synthetic fundamental magnetomotive forces under 20 different arrangement modes were obtained. The results show that the synthetic magnetomotive force with d = 2 and e = 4 is close to forward sinusoidal traveling wave and the synthetic magnetomotive force with d = 4 and e = 2 is close to backward sinusoidal traveling wave, and their amplitudes and wave velocities are approximately constant and equal. In both cases, the motor could work normally with ahigh efficiency, but under other 18 arrangement modes (d= 1, e=2; d= 1, e=3; d= 1, e=4;...), the synthetic magnetomotive force presents obvious pulse vibration and moves with variable velocity, which means that the motor did not work normally and had high energy loss. |
doi_str_mv | 10.1007/s40534-013-0018-7 |
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The ideal model of the cascaded linear induction motor was built, in which the B and C-phase windings are respectively separated from the A-phase winding by a distance of d and e slots pitch and not overlapped. By changing the values of d and e from 1 to 5, we can obtain 20 different modes of three-phase winding with the different combinations of d and e. Then, the air-gap magnetomotive forces of A-, B-, and C-phase windings were calculated by the magnetomotive force theory. According to the transient superposition of magnetomotive forces of A-, B-, and C-phase windings, the theoretical and simulated synthetic fundamental magnetomotive forces under 20 different arrangement modes were obtained. The results show that the synthetic magnetomotive force with d = 2 and e = 4 is close to forward sinusoidal traveling wave and the synthetic magnetomotive force with d = 4 and e = 2 is close to backward sinusoidal traveling wave, and their amplitudes and wave velocities are approximately constant and equal. In both cases, the motor could work normally with ahigh efficiency, but under other 18 arrangement modes (d= 1, e=2; d= 1, e=3; d= 1, e=4;...), the synthetic magnetomotive force presents obvious pulse vibration and moves with variable velocity, which means that the motor did not work normally and had high energy loss.</description><identifier>ISSN: 2095-087X</identifier><identifier>ISSN: 2662-4745</identifier><identifier>EISSN: 2196-0577</identifier><identifier>EISSN: 2662-4753</identifier><identifier>DOI: 10.1007/s40534-013-0018-7</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Automotive Engineering ; Constants ; Energy loss ; Engineering ; Foundations ; Geoengineering ; Hydraulics ; Induction motors ; Mathematical models ; Motors ; Regional/Spatial Science ; Transportation ; Traveling waves ; Vibration ; Wave velocity ; Winding ; 三相绕组 ; 和空间 ; 时间 ; 特性 ; 直线感应电动机 ; 直线感应电机 ; 磁通势 ; 级联</subject><ispartof>Journal of modern transportation, 2013-09, Vol.21 (3), p.194-199</ispartof><rights>The Author(s) 2013</rights><rights>Copyright © Wanfang Data Co. Ltd. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c406t-4df8fb36b28f2ba6b6fe3827a5ec935ac0b3b708e7521b88a9cdd130b4669b203</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://image.cqvip.com/vip1000/qk/85396A/85396A.jpg</thumbnail><link.rule.ids>314,780,784,864,27923,27924</link.rule.ids></links><search><creatorcontrib>Zhou, Dajing</creatorcontrib><creatorcontrib>Ma, Jiaqing</creatorcontrib><creatorcontrib>Zhao, Lifeng</creatorcontrib><creatorcontrib>Wan, Xiao</creatorcontrib><creatorcontrib>Zhang, Yong</creatorcontrib><creatorcontrib>Zhao, Yong</creatorcontrib><title>The time and space characteristics of magnetomotive force in the cascaded linear induction motor</title><title>Journal of modern transportation</title><addtitle>J. Mod. Transport</addtitle><addtitle>Journal of Modern Transportation</addtitle><description>To choose a reasonable mode of three-phase winding for the improvement of the operating efficiency of cascaded linear induction motor, the time and space characteristics of magnetomotive force were investigated. The ideal model of the cascaded linear induction motor was built, in which the B and C-phase windings are respectively separated from the A-phase winding by a distance of d and e slots pitch and not overlapped. By changing the values of d and e from 1 to 5, we can obtain 20 different modes of three-phase winding with the different combinations of d and e. Then, the air-gap magnetomotive forces of A-, B-, and C-phase windings were calculated by the magnetomotive force theory. According to the transient superposition of magnetomotive forces of A-, B-, and C-phase windings, the theoretical and simulated synthetic fundamental magnetomotive forces under 20 different arrangement modes were obtained. The results show that the synthetic magnetomotive force with d = 2 and e = 4 is close to forward sinusoidal traveling wave and the synthetic magnetomotive force with d = 4 and e = 2 is close to backward sinusoidal traveling wave, and their amplitudes and wave velocities are approximately constant and equal. In both cases, the motor could work normally with ahigh efficiency, but under other 18 arrangement modes (d= 1, e=2; d= 1, e=3; d= 1, e=4;...), the synthetic magnetomotive force presents obvious pulse vibration and moves with variable velocity, which means that the motor did not work normally and had high energy loss.</description><subject>Automotive Engineering</subject><subject>Constants</subject><subject>Energy loss</subject><subject>Engineering</subject><subject>Foundations</subject><subject>Geoengineering</subject><subject>Hydraulics</subject><subject>Induction motors</subject><subject>Mathematical models</subject><subject>Motors</subject><subject>Regional/Spatial Science</subject><subject>Transportation</subject><subject>Traveling waves</subject><subject>Vibration</subject><subject>Wave velocity</subject><subject>Winding</subject><subject>三相绕组</subject><subject>和空间</subject><subject>时间</subject><subject>特性</subject><subject>直线感应电动机</subject><subject>直线感应电机</subject><subject>磁通势</subject><subject>级联</subject><issn>2095-087X</issn><issn>2662-4745</issn><issn>2196-0577</issn><issn>2662-4753</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp9kU9rFTEUxQdRsNR-AHcRN4JMvUkmf2YpxapQcFPBXUwyN-_N403ymuTZ57c3ZUoRF65uuPzOOZecrntN4ZICqA9lAMGHHijvAaju1bPujNFR9iCUet7eMIoetPrxsrsoZQcNklIyoc-6n7dbJHVekNg4kXKwHonf2mx9xTyXOvtCUiCL3USsaUl1_oUkpNywOZLaxN4WbyecyH6OaHNbT0df5xRJo1N-1b0Idl_w4nGed9-vP91efelvvn3-evXxpvcDyNoPU9DBcemYDsxZ6WRArpmyAv3IhfXguFOgUQlGndZ29NNEObhBytEx4Ofd-9X33sZg48bs0jHHlmhOcVen08kZZO2HgAPIRr9b6UNOd0cs1Sxz8bjf24jpWAxVWlIl1CAa-vYf9MmZSsFGNYySN4qulM-plIzBHPK82PzbUDAPJZm1JNNOMA8lGdU0bNWUxsYN5r-c_yN68xi0TXFz13RPSYNijAvG-R-3ip9t</recordid><startdate>20130901</startdate><enddate>20130901</enddate><creator>Zhou, Dajing</creator><creator>Ma, Jiaqing</creator><creator>Zhao, Lifeng</creator><creator>Wan, Xiao</creator><creator>Zhang, Yong</creator><creator>Zhao, Yong</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><general>Superconductivity and New Energy R&D Center, Southwest Jiaotong University, Chengdu 610031, Sichuan, China%Key Laboratory of Magnetic Levitation Technologies and Maglev Trains(Ministry of Education of China), Southwest Jiaotong University, Chengdu 610031, Sichuan, China</general><general>School of Materials Science and Engineering, University of New South Wales, Sydney, NSW 2052, Australia</general><general>Key Laboratory of Magnetic Levitation Technologies and Maglev Trains(Ministry of Education of China), Southwest Jiaotong University, Chengdu 610031, Sichuan, China</general><general>Superconductivity and New Energy R&D Center, Southwest Jiaotong University, Chengdu 610031, Sichuan, China</general><scope>2RA</scope><scope>92L</scope><scope>CQIGP</scope><scope>W92</scope><scope>~WA</scope><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PTHSS</scope><scope>7SU</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>KR7</scope><scope>2B.</scope><scope>4A8</scope><scope>92I</scope><scope>93N</scope><scope>PSX</scope><scope>TCJ</scope></search><sort><creationdate>20130901</creationdate><title>The time and space characteristics of magnetomotive force in the cascaded linear induction motor</title><author>Zhou, Dajing ; 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Mod. Transport</stitle><addtitle>Journal of Modern Transportation</addtitle><date>2013-09-01</date><risdate>2013</risdate><volume>21</volume><issue>3</issue><spage>194</spage><epage>199</epage><pages>194-199</pages><issn>2095-087X</issn><issn>2662-4745</issn><eissn>2196-0577</eissn><eissn>2662-4753</eissn><abstract>To choose a reasonable mode of three-phase winding for the improvement of the operating efficiency of cascaded linear induction motor, the time and space characteristics of magnetomotive force were investigated. The ideal model of the cascaded linear induction motor was built, in which the B and C-phase windings are respectively separated from the A-phase winding by a distance of d and e slots pitch and not overlapped. By changing the values of d and e from 1 to 5, we can obtain 20 different modes of three-phase winding with the different combinations of d and e. Then, the air-gap magnetomotive forces of A-, B-, and C-phase windings were calculated by the magnetomotive force theory. According to the transient superposition of magnetomotive forces of A-, B-, and C-phase windings, the theoretical and simulated synthetic fundamental magnetomotive forces under 20 different arrangement modes were obtained. The results show that the synthetic magnetomotive force with d = 2 and e = 4 is close to forward sinusoidal traveling wave and the synthetic magnetomotive force with d = 4 and e = 2 is close to backward sinusoidal traveling wave, and their amplitudes and wave velocities are approximately constant and equal. In both cases, the motor could work normally with ahigh efficiency, but under other 18 arrangement modes (d= 1, e=2; d= 1, e=3; d= 1, e=4;...), the synthetic magnetomotive force presents obvious pulse vibration and moves with variable velocity, which means that the motor did not work normally and had high energy loss.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/s40534-013-0018-7</doi><tpages>6</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Automotive Engineering Constants Energy loss Engineering Foundations Geoengineering Hydraulics Induction motors Mathematical models Motors Regional/Spatial Science Transportation Traveling waves Vibration Wave velocity Winding 三相绕组 和空间 时间 特性 直线感应电动机 直线感应电机 磁通势 级联 |
title | The time and space characteristics of magnetomotive force in the cascaded linear induction motor |
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