F. Najmabadi, R. Conn, C. Bathke, J. Blanchard, L. Bromberg, J. Brooks, E. Cheng, D. Cohn, D. Ehst, L. El-Guebaly, G. Emmert, T. Dolan, P. Gierszewski, S. Grotz, M.S. Hasan, J. Herring, S. K. Ho, A. Hollies, J. Holmes, E. Ibrahim, S. Jardin, C. Kessel, H. Khater, R. Krakowski, G.L. Kuleinski, J. Mandrekas, T. Mau, G. Miley, R.L. Miller, E. Mogahed, E. Reis, J. Santarius, M. Sawan, J. Schultz, K. Schultz, S. Sharafat, D. Steiner, D. Strickler, I. Sviatoslavsky, D. Sze, P. Titus, M. Valenti, K. Werley, J. H. Whealton, J.E.C. Williams, L. Wittenberg, C. Wong
{"title":"白羊座- iii D-3He托卡马克反应堆研究","authors":"F. Najmabadi, R. Conn, C. Bathke, J. Blanchard, L. Bromberg, J. Brooks, E. Cheng, D. Cohn, D. Ehst, L. El-Guebaly, G. Emmert, T. Dolan, P. Gierszewski, S. Grotz, M.S. Hasan, J. Herring, S. K. Ho, A. Hollies, J. Holmes, E. Ibrahim, S. Jardin, C. Kessel, H. Khater, R. Krakowski, G.L. Kuleinski, J. Mandrekas, T. Mau, G. Miley, R.L. Miller, E. Mogahed, E. Reis, J. Santarius, M. Sawan, J. Schultz, K. Schultz, S. Sharafat, D. Steiner, D. Strickler, I. Sviatoslavsky, D. Sze, P. Titus, M. Valenti, K. Werley, J. H. Whealton, J.E.C. Williams, L. Wittenberg, C. Wong","doi":"10.1109/FUSION.1991.218914","DOIUrl":null,"url":null,"abstract":"A description of the ARIES-III research effort is presented, and the general features of the ARIES-III reactor are described. The plasma engineering and fusion-power-core design are summarized, including the major results, the key technical issues, and the central conclusions. Analyses have shown that the plasma power-balance window for D-/sup 3/He tokamak reactors is small and requires a first wall (or coating) that is highly reflective to synchrotron radiation and small values of tau /sub ash// epsilon /sub e/ (the ratio of ash-particle to energy confinement times in the core plasma). Both first and second stability regimes of operation have been considered. The second stability regime is chosen for the ARIES-III design point because the reactor can operate at a higher value of tau /sub ash// tau /sub E// tau /sub E/ approximately=2 (twice that of a first stability version), and because it has a reduced plasma current (30 MA), magnetic field at the coil (14 T), mass, and cost (also compared to a first-stability D-/sup 3/He reactor). The major and minor radii are, respectively 7.5 and 2.5 m.<<ETX>>","PeriodicalId":318951,"journal":{"name":"[Proceedings] The 14th IEEE/NPSS Symposium Fusion Engineering","volume":"11 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1991-09-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"22","resultStr":"{\"title\":\"The ARIES-III D-3He tokamak-reactor study\",\"authors\":\"F. Najmabadi, R. Conn, C. Bathke, J. Blanchard, L. Bromberg, J. Brooks, E. Cheng, D. Cohn, D. Ehst, L. El-Guebaly, G. Emmert, T. Dolan, P. Gierszewski, S. Grotz, M.S. Hasan, J. Herring, S. K. Ho, A. Hollies, J. Holmes, E. Ibrahim, S. Jardin, C. Kessel, H. Khater, R. Krakowski, G.L. Kuleinski, J. Mandrekas, T. Mau, G. Miley, R.L. Miller, E. Mogahed, E. Reis, J. Santarius, M. Sawan, J. Schultz, K. Schultz, S. Sharafat, D. Steiner, D. Strickler, I. Sviatoslavsky, D. Sze, P. Titus, M. Valenti, K. Werley, J. H. Whealton, J.E.C. Williams, L. Wittenberg, C. Wong\",\"doi\":\"10.1109/FUSION.1991.218914\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A description of the ARIES-III research effort is presented, and the general features of the ARIES-III reactor are described. The plasma engineering and fusion-power-core design are summarized, including the major results, the key technical issues, and the central conclusions. Analyses have shown that the plasma power-balance window for D-/sup 3/He tokamak reactors is small and requires a first wall (or coating) that is highly reflective to synchrotron radiation and small values of tau /sub ash// epsilon /sub e/ (the ratio of ash-particle to energy confinement times in the core plasma). Both first and second stability regimes of operation have been considered. The second stability regime is chosen for the ARIES-III design point because the reactor can operate at a higher value of tau /sub ash// tau /sub E// tau /sub E/ approximately=2 (twice that of a first stability version), and because it has a reduced plasma current (30 MA), magnetic field at the coil (14 T), mass, and cost (also compared to a first-stability D-/sup 3/He reactor). The major and minor radii are, respectively 7.5 and 2.5 m.<<ETX>>\",\"PeriodicalId\":318951,\"journal\":{\"name\":\"[Proceedings] The 14th IEEE/NPSS Symposium Fusion Engineering\",\"volume\":\"11 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1991-09-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"22\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"[Proceedings] The 14th IEEE/NPSS Symposium Fusion Engineering\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/FUSION.1991.218914\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"[Proceedings] The 14th IEEE/NPSS Symposium Fusion Engineering","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/FUSION.1991.218914","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A description of the ARIES-III research effort is presented, and the general features of the ARIES-III reactor are described. The plasma engineering and fusion-power-core design are summarized, including the major results, the key technical issues, and the central conclusions. Analyses have shown that the plasma power-balance window for D-/sup 3/He tokamak reactors is small and requires a first wall (or coating) that is highly reflective to synchrotron radiation and small values of tau /sub ash// epsilon /sub e/ (the ratio of ash-particle to energy confinement times in the core plasma). Both first and second stability regimes of operation have been considered. The second stability regime is chosen for the ARIES-III design point because the reactor can operate at a higher value of tau /sub ash// tau /sub E// tau /sub E/ approximately=2 (twice that of a first stability version), and because it has a reduced plasma current (30 MA), magnetic field at the coil (14 T), mass, and cost (also compared to a first-stability D-/sup 3/He reactor). The major and minor radii are, respectively 7.5 and 2.5 m.<>
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