Numerical study of plasma behavior in a disk‐shaped noble gas MHD generator
Plasma behavior in cesium‐seeded argon (Ar/Cs) and xenon‐seeded argon (Ar/Xe) disk‐shaped MHD generators are compared under almost the same working conditions using r‐θ two‐dimensional simulation. For both working gases, uniform plasma occurs at the optimum load resistance, and the power outputs are...
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Veröffentlicht in: | Electronics and communications in Japan 2024-06, Vol.107 (2), p.n/a |
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description | Plasma behavior in cesium‐seeded argon (Ar/Cs) and xenon‐seeded argon (Ar/Xe) disk‐shaped MHD generators are compared under almost the same working conditions using r‐θ two‐dimensional simulation. For both working gases, uniform plasma occurs at the optimum load resistance, and the power outputs are the same under an identical inlet ionization degree. For Ar/Cs, plasma is stable and uniform in the range of electron temperature of 4300–5800 K basically according to the linear perturbation theory. In the actual plasma in the MHD generator, however, the uniform plasma still can be maintained even at higher electron temperatures due to the low three‐body recombination coefficient of Ar. For Ar/Xe, on the other hand, uniform plasma is maintained when the characteristic time of the electron number density is longer than the residence time of the working gas where the electron temperature is around 4300–8600 K, even though unstable plasma is suggested from the linear perturbation theory. |
doi_str_mv | 10.1002/ecj.12445 |
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For both working gases, uniform plasma occurs at the optimum load resistance, and the power outputs are the same under an identical inlet ionization degree. For Ar/Cs, plasma is stable and uniform in the range of electron temperature of 4300–5800 K basically according to the linear perturbation theory. In the actual plasma in the MHD generator, however, the uniform plasma still can be maintained even at higher electron temperatures due to the low three‐body recombination coefficient of Ar. For Ar/Xe, on the other hand, uniform plasma is maintained when the characteristic time of the electron number density is longer than the residence time of the working gas where the electron temperature is around 4300–8600 K, even though unstable plasma is suggested from the linear perturbation theory.</description><identifier>ISSN: 1942-9533</identifier><identifier>EISSN: 1942-9541</identifier><identifier>DOI: 10.1002/ecj.12445</identifier><language>eng</language><publisher>Hoboken: Wiley Subscription Services, Inc</publisher><subject>Argon ; Cesium ; disk‐shaped generator ; Electron energy ; Electrons ; Load resistance ; Magnetohydrodynamic generators ; MHD electrical power generation ; numerical simulation ; Perturbation theory ; Plasma ; plasma behavior ; Rare gases ; Recombination coefficient ; seeded plasma ; Xenon</subject><ispartof>Electronics and communications in Japan, 2024-06, Vol.107 (2), p.n/a</ispartof><rights>2024 Wiley Periodicals LLC.</rights><rights>2024 by Wiley Periodicals LLC.</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c2535-93238a8ed9a10080e8269ff3590f773eef6b687f8f9086affd3de060cc65fde93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fecj.12445$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fecj.12445$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,777,781,1412,27905,27906,45555,45556</link.rule.ids></links><search><creatorcontrib>Kimsor, Ork</creatorcontrib><creatorcontrib>Okuno, Yoshihiro</creatorcontrib><title>Numerical study of plasma behavior in a disk‐shaped noble gas MHD generator</title><title>Electronics and communications in Japan</title><description>Plasma behavior in cesium‐seeded argon (Ar/Cs) and xenon‐seeded argon (Ar/Xe) disk‐shaped MHD generators are compared under almost the same working conditions using r‐θ two‐dimensional simulation. For both working gases, uniform plasma occurs at the optimum load resistance, and the power outputs are the same under an identical inlet ionization degree. For Ar/Cs, plasma is stable and uniform in the range of electron temperature of 4300–5800 K basically according to the linear perturbation theory. In the actual plasma in the MHD generator, however, the uniform plasma still can be maintained even at higher electron temperatures due to the low three‐body recombination coefficient of Ar. For Ar/Xe, on the other hand, uniform plasma is maintained when the characteristic time of the electron number density is longer than the residence time of the working gas where the electron temperature is around 4300–8600 K, even though unstable plasma is suggested from the linear perturbation theory.</description><subject>Argon</subject><subject>Cesium</subject><subject>disk‐shaped generator</subject><subject>Electron energy</subject><subject>Electrons</subject><subject>Load resistance</subject><subject>Magnetohydrodynamic generators</subject><subject>MHD electrical power generation</subject><subject>numerical simulation</subject><subject>Perturbation theory</subject><subject>Plasma</subject><subject>plasma behavior</subject><subject>Rare gases</subject><subject>Recombination coefficient</subject><subject>seeded plasma</subject><subject>Xenon</subject><issn>1942-9533</issn><issn>1942-9541</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp1kL1OwzAQxy0EEqUw8AaWmBjS2vFH4hGVj4JaWGC23PjcpqRJsBtQNx6BZ-RJMASxMd0Nv7v_3Q-hU0pGlJB0DMV6RFPOxR4aUMXTRAlO9_96xg7RUQhrQiQXnA3Q_L7bgC8LU-Gw7ewONw63lQkbgxewMq9l43FZY4NtGZ4_3z_CyrRgcd0sKsBLE_B8eomXUIM328YfowNnqgAnv3WInq6vHifTZPZwczu5mCVFKphIFEtZbnKwysSjcwJ5KpVzTCjisowBOLmQeeZyp0gujXOWWSCSFIUUzoJiQ3TW721989JB2Op10_k6RmoWP-M0pmSROu-pwjcheHC69eXG-J2mRH_b0tGW_rEV2XHPvpUV7P4H9dXkrp_4Ag6Ra4Q</recordid><startdate>202406</startdate><enddate>202406</enddate><creator>Kimsor, Ork</creator><creator>Okuno, Yoshihiro</creator><general>Wiley Subscription Services, Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SC</scope><scope>7SP</scope><scope>8FD</scope><scope>JQ2</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope></search><sort><creationdate>202406</creationdate><title>Numerical study of plasma behavior in a disk‐shaped noble gas MHD generator</title><author>Kimsor, Ork ; Okuno, Yoshihiro</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2535-93238a8ed9a10080e8269ff3590f773eef6b687f8f9086affd3de060cc65fde93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Argon</topic><topic>Cesium</topic><topic>disk‐shaped generator</topic><topic>Electron energy</topic><topic>Electrons</topic><topic>Load resistance</topic><topic>Magnetohydrodynamic generators</topic><topic>MHD electrical power generation</topic><topic>numerical simulation</topic><topic>Perturbation theory</topic><topic>Plasma</topic><topic>plasma behavior</topic><topic>Rare gases</topic><topic>Recombination coefficient</topic><topic>seeded plasma</topic><topic>Xenon</topic><toplevel>online_resources</toplevel><creatorcontrib>Kimsor, Ork</creatorcontrib><creatorcontrib>Okuno, Yoshihiro</creatorcontrib><collection>CrossRef</collection><collection>Computer and Information Systems Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><jtitle>Electronics and communications in Japan</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kimsor, Ork</au><au>Okuno, Yoshihiro</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Numerical study of plasma behavior in a disk‐shaped noble gas MHD generator</atitle><jtitle>Electronics and communications in Japan</jtitle><date>2024-06</date><risdate>2024</risdate><volume>107</volume><issue>2</issue><epage>n/a</epage><issn>1942-9533</issn><eissn>1942-9541</eissn><abstract>Plasma behavior in cesium‐seeded argon (Ar/Cs) and xenon‐seeded argon (Ar/Xe) disk‐shaped MHD generators are compared under almost the same working conditions using r‐θ two‐dimensional simulation. For both working gases, uniform plasma occurs at the optimum load resistance, and the power outputs are the same under an identical inlet ionization degree. For Ar/Cs, plasma is stable and uniform in the range of electron temperature of 4300–5800 K basically according to the linear perturbation theory. In the actual plasma in the MHD generator, however, the uniform plasma still can be maintained even at higher electron temperatures due to the low three‐body recombination coefficient of Ar. For Ar/Xe, on the other hand, uniform plasma is maintained when the characteristic time of the electron number density is longer than the residence time of the working gas where the electron temperature is around 4300–8600 K, even though unstable plasma is suggested from the linear perturbation theory.</abstract><cop>Hoboken</cop><pub>Wiley Subscription Services, Inc</pub><doi>10.1002/ecj.12445</doi><tpages>8</tpages></addata></record> |
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subjects | Argon Cesium disk‐shaped generator Electron energy Electrons Load resistance Magnetohydrodynamic generators MHD electrical power generation numerical simulation Perturbation theory Plasma plasma behavior Rare gases Recombination coefficient seeded plasma Xenon |
title | Numerical study of plasma behavior in a disk‐shaped noble gas MHD generator |
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