Optimization of Electrodynamic Energy Transfer in Coilguns With Multiple, Uncoupled Stages
A 1-D model for inductive electromagnetic acceleration of projectiles using a coilgun has been nondimensionalized to find relevant scaling parameters. The dynamic impedance parameter, representing the ratio of the resonant period of the unloaded electrical circuit to the time the projectile is elect...
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Veröffentlicht in: | IEEE transactions on magnetics 2013-04, Vol.49 (4), p.1453-1460 |
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description | A 1-D model for inductive electromagnetic acceleration of projectiles using a coilgun has been nondimensionalized to find relevant scaling parameters. The dynamic impedance parameter, representing the ratio of the resonant period of the unloaded electrical circuit to the time the projectile is electromagnetically coupled to the coil, is the scaling term that can be adjusted to optimize the electromagnetic energy transfer process. The mutual inductance profile, which represents the ability to convert potential electromagnetic energy into projectile kinetic energy, was modeled for a specific geometry using a semi-empirical function previously found suitable for cylindrical pulsed inductive plasma accelerators. Contour plots representing coilgun efficiency were generated for varying initial projectile velocity across a range of dynamic impedances. The contour plots show that below a given initial velocity a dynamic impedance parameter can be selected to maximize energy transfer to the projectile. This optimum varies as a function of the initial velocity a projectile possessed when it enters the coilgun stage. Once the contour plot is generated for a geometry it can be used to optimize the acceleration process for any stage in a coilgun if the individual coils comprising the stages are electromagnetically uncoupled from each other and the velocity of the projectile as it exits the previous stage is known. |
doi_str_mv | 10.1109/TMAG.2012.2230271 |
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The dynamic impedance parameter, representing the ratio of the resonant period of the unloaded electrical circuit to the time the projectile is electromagnetically coupled to the coil, is the scaling term that can be adjusted to optimize the electromagnetic energy transfer process. The mutual inductance profile, which represents the ability to convert potential electromagnetic energy into projectile kinetic energy, was modeled for a specific geometry using a semi-empirical function previously found suitable for cylindrical pulsed inductive plasma accelerators. Contour plots representing coilgun efficiency were generated for varying initial projectile velocity across a range of dynamic impedances. The contour plots show that below a given initial velocity a dynamic impedance parameter can be selected to maximize energy transfer to the projectile. This optimum varies as a function of the initial velocity a projectile possessed when it enters the coilgun stage. Once the contour plot is generated for a geometry it can be used to optimize the acceleration process for any stage in a coilgun if the individual coils comprising the stages are electromagnetically uncoupled from each other and the velocity of the projectile as it exits the previous stage is known.</description><identifier>ISSN: 0018-9464</identifier><identifier>EISSN: 1941-0069</identifier><identifier>DOI: 10.1109/TMAG.2012.2230271</identifier><identifier>CODEN: IEMGAQ</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Acceleration ; Coilgun ; Coilguns ; Coils ; Cross-disciplinary physics: materials science; rheology ; Exact sciences and technology ; Inductance ; inductive accelerators ; Integrated circuit modeling ; Materials science ; Mathematical model ; modeling ; optimization ; Other topics in materials science ; Physics ; Projectiles</subject><ispartof>IEEE transactions on magnetics, 2013-04, Vol.49 (4), p.1453-1460</ispartof><rights>2014 INIST-CNRS</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c295t-5e189997cc53522cfd249aa0984920a8a4ab5aa23e6aa848bc9f05e0655563fd3</citedby><cites>FETCH-LOGICAL-c295t-5e189997cc53522cfd249aa0984920a8a4ab5aa23e6aa848bc9f05e0655563fd3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/6363606$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,792,27903,27904,54737</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/6363606$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=27211163$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Polzin, Kurt A.</creatorcontrib><creatorcontrib>Adwar, Jake E.</creatorcontrib><creatorcontrib>Hallock, Ashley K.</creatorcontrib><title>Optimization of Electrodynamic Energy Transfer in Coilguns With Multiple, Uncoupled Stages</title><title>IEEE transactions on magnetics</title><addtitle>TMAG</addtitle><description>A 1-D model for inductive electromagnetic acceleration of projectiles using a coilgun has been nondimensionalized to find relevant scaling parameters. The dynamic impedance parameter, representing the ratio of the resonant period of the unloaded electrical circuit to the time the projectile is electromagnetically coupled to the coil, is the scaling term that can be adjusted to optimize the electromagnetic energy transfer process. The mutual inductance profile, which represents the ability to convert potential electromagnetic energy into projectile kinetic energy, was modeled for a specific geometry using a semi-empirical function previously found suitable for cylindrical pulsed inductive plasma accelerators. Contour plots representing coilgun efficiency were generated for varying initial projectile velocity across a range of dynamic impedances. The contour plots show that below a given initial velocity a dynamic impedance parameter can be selected to maximize energy transfer to the projectile. This optimum varies as a function of the initial velocity a projectile possessed when it enters the coilgun stage. Once the contour plot is generated for a geometry it can be used to optimize the acceleration process for any stage in a coilgun if the individual coils comprising the stages are electromagnetically uncoupled from each other and the velocity of the projectile as it exits the previous stage is known.</description><subject>Acceleration</subject><subject>Coilgun</subject><subject>Coilguns</subject><subject>Coils</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Exact sciences and technology</subject><subject>Inductance</subject><subject>inductive accelerators</subject><subject>Integrated circuit modeling</subject><subject>Materials science</subject><subject>Mathematical model</subject><subject>modeling</subject><subject>optimization</subject><subject>Other topics in materials science</subject><subject>Physics</subject><subject>Projectiles</subject><issn>0018-9464</issn><issn>1941-0069</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kE9PAjEQxRujiYh-AOOlF28udvqP7ZEQRBMIByEmXjZDt8WaZZe0ywE_vUsgZA4zk3nvJfMj5BHYAICZ1-V8NB1wBnzAuWB8CFekB0ZCxpg216THGOSZkVrekruUfrtVKmA98r3YtWEb_rANTU0bTyeVs21sykON22DppHZxc6DLiHXyLtJQ03ETqs2-TvQrtD90vq_asKvcC13Vttl3U0k_W9y4dE9uPFbJPZx7n6zeJsvxezZbTD_Go1lmuVFtphzkxpihtUoozq0vuTSIzOTScIY5SlwrRC6cRsxlvrbGM-WYVkpp4UvRJ3DKtbFJKTpf7GLYYjwUwIojnOIIpzjCKc5wOs_zybPDZLHy3Xs2pIuRDzkAaNHpnk664Jy7nLXoimnxD-WXbfk</recordid><startdate>20130401</startdate><enddate>20130401</enddate><creator>Polzin, Kurt A.</creator><creator>Adwar, Jake E.</creator><creator>Hallock, Ashley K.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20130401</creationdate><title>Optimization of Electrodynamic Energy Transfer in Coilguns With Multiple, Uncoupled Stages</title><author>Polzin, Kurt A. ; Adwar, Jake E. ; Hallock, Ashley K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c295t-5e189997cc53522cfd249aa0984920a8a4ab5aa23e6aa848bc9f05e0655563fd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Acceleration</topic><topic>Coilgun</topic><topic>Coilguns</topic><topic>Coils</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Exact sciences and technology</topic><topic>Inductance</topic><topic>inductive accelerators</topic><topic>Integrated circuit modeling</topic><topic>Materials science</topic><topic>Mathematical model</topic><topic>modeling</topic><topic>optimization</topic><topic>Other topics in materials science</topic><topic>Physics</topic><topic>Projectiles</topic><toplevel>online_resources</toplevel><creatorcontrib>Polzin, Kurt A.</creatorcontrib><creatorcontrib>Adwar, Jake E.</creatorcontrib><creatorcontrib>Hallock, Ashley K.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Xplore (Online service)</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>IEEE transactions on magnetics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Polzin, Kurt A.</au><au>Adwar, Jake E.</au><au>Hallock, Ashley K.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optimization of Electrodynamic Energy Transfer in Coilguns With Multiple, Uncoupled Stages</atitle><jtitle>IEEE transactions on magnetics</jtitle><stitle>TMAG</stitle><date>2013-04-01</date><risdate>2013</risdate><volume>49</volume><issue>4</issue><spage>1453</spage><epage>1460</epage><pages>1453-1460</pages><issn>0018-9464</issn><eissn>1941-0069</eissn><coden>IEMGAQ</coden><abstract>A 1-D model for inductive electromagnetic acceleration of projectiles using a coilgun has been nondimensionalized to find relevant scaling parameters. The dynamic impedance parameter, representing the ratio of the resonant period of the unloaded electrical circuit to the time the projectile is electromagnetically coupled to the coil, is the scaling term that can be adjusted to optimize the electromagnetic energy transfer process. The mutual inductance profile, which represents the ability to convert potential electromagnetic energy into projectile kinetic energy, was modeled for a specific geometry using a semi-empirical function previously found suitable for cylindrical pulsed inductive plasma accelerators. Contour plots representing coilgun efficiency were generated for varying initial projectile velocity across a range of dynamic impedances. The contour plots show that below a given initial velocity a dynamic impedance parameter can be selected to maximize energy transfer to the projectile. This optimum varies as a function of the initial velocity a projectile possessed when it enters the coilgun stage. Once the contour plot is generated for a geometry it can be used to optimize the acceleration process for any stage in a coilgun if the individual coils comprising the stages are electromagnetically uncoupled from each other and the velocity of the projectile as it exits the previous stage is known.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TMAG.2012.2230271</doi><tpages>8</tpages></addata></record> |
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subjects | Acceleration Coilgun Coilguns Coils Cross-disciplinary physics: materials science rheology Exact sciences and technology Inductance inductive accelerators Integrated circuit modeling Materials science Mathematical model modeling optimization Other topics in materials science Physics Projectiles |
title | Optimization of Electrodynamic Energy Transfer in Coilguns With Multiple, Uncoupled Stages |
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