Characteristics of transient plasma layers produced by irradiation of graphite targets by high power quasi-stationary plasma streams under the disruption simulation conditions
Simulation experiments to model the situation occurring at the divertor plates during disruptions and ELMy H-modes of tokamak were carried out with plasma streams generated at the Kharkov QSPA. The facility ultimate plasma parameters were as follows: plasma energy density — above 2 kJ/cm 2, proton e...
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Veröffentlicht in: | Journal of nuclear materials 1996-10, Vol.233 (1-3), p.736-740 |
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creator | Chebotarev, V.V. Garkusha, I.E. Garkusha, V.V. Makhlaj, V.A. Mitina, N.I. Solyakov, D.G. Tereshin, V.I. Trubchaninov, S.A. Tsarenko, A.V. Wuerz, H. |
description | Simulation experiments to model the situation occurring at the divertor plates during disruptions and ELMy H-modes of tokamak were carried out with plasma streams generated at the Kharkov QSPA. The facility ultimate plasma parameters were as follows: plasma energy density — above 2 kJ/cm
2, proton energy — 0.9 keV, plasma density — 10
16 cm
−3, pulse duration — 0.1–0.15 ms. Graphite targets of different sizes utilized in these experiments. It was shown that high density target plasma layer, with densities up to 6 · 10
17 cm
−3, were formed above the target surface, when incident plasma interacted with target, and sustained during the whole pulse. Density and thickness (usually within 3 to 5 cm) increased with increasing incident plasma power and target surface. The main part of incident plasma energy (≈ 90%) is absorbed by the transient layer on the first 2–3 cm of its thickness. The average erosion coefficient of the graphite under the influence of incident plasma was of the order of 1 μm/kJ. |
doi_str_mv | 10.1016/S0022-3115(96)00329-7 |
format | Article |
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2, proton energy — 0.9 keV, plasma density — 10
16 cm
−3, pulse duration — 0.1–0.15 ms. Graphite targets of different sizes utilized in these experiments. It was shown that high density target plasma layer, with densities up to 6 · 10
17 cm
−3, were formed above the target surface, when incident plasma interacted with target, and sustained during the whole pulse. Density and thickness (usually within 3 to 5 cm) increased with increasing incident plasma power and target surface. The main part of incident plasma energy (≈ 90%) is absorbed by the transient layer on the first 2–3 cm of its thickness. The average erosion coefficient of the graphite under the influence of incident plasma was of the order of 1 μm/kJ.</description><identifier>ISSN: 0022-3115</identifier><identifier>EISSN: 1873-4820</identifier><identifier>DOI: 10.1016/S0022-3115(96)00329-7</identifier><language>eng</language><publisher>Elsevier B.V</publisher><ispartof>Journal of nuclear materials, 1996-10, Vol.233 (1-3), p.736-740</ispartof><rights>1996</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c404t-f32adcab91cf0d2f3a4cb634b59a7ad2550543c3e9d5192c2f7441c62d3342f83</citedby><cites>FETCH-LOGICAL-c404t-f32adcab91cf0d2f3a4cb634b59a7ad2550543c3e9d5192c2f7441c62d3342f83</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0022311596003297$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids></links><search><creatorcontrib>Chebotarev, V.V.</creatorcontrib><creatorcontrib>Garkusha, I.E.</creatorcontrib><creatorcontrib>Garkusha, V.V.</creatorcontrib><creatorcontrib>Makhlaj, V.A.</creatorcontrib><creatorcontrib>Mitina, N.I.</creatorcontrib><creatorcontrib>Solyakov, D.G.</creatorcontrib><creatorcontrib>Tereshin, V.I.</creatorcontrib><creatorcontrib>Trubchaninov, S.A.</creatorcontrib><creatorcontrib>Tsarenko, A.V.</creatorcontrib><creatorcontrib>Wuerz, H.</creatorcontrib><title>Characteristics of transient plasma layers produced by irradiation of graphite targets by high power quasi-stationary plasma streams under the disruption simulation conditions</title><title>Journal of nuclear materials</title><description>Simulation experiments to model the situation occurring at the divertor plates during disruptions and ELMy H-modes of tokamak were carried out with plasma streams generated at the Kharkov QSPA. The facility ultimate plasma parameters were as follows: plasma energy density — above 2 kJ/cm
2, proton energy — 0.9 keV, plasma density — 10
16 cm
−3, pulse duration — 0.1–0.15 ms. Graphite targets of different sizes utilized in these experiments. It was shown that high density target plasma layer, with densities up to 6 · 10
17 cm
−3, were formed above the target surface, when incident plasma interacted with target, and sustained during the whole pulse. Density and thickness (usually within 3 to 5 cm) increased with increasing incident plasma power and target surface. The main part of incident plasma energy (≈ 90%) is absorbed by the transient layer on the first 2–3 cm of its thickness. The average erosion coefficient of the graphite under the influence of incident plasma was of the order of 1 μm/kJ.</description><issn>0022-3115</issn><issn>1873-4820</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNqFkUurFDEUhIMoOF79CUJWoovWPLsnK5Hh-oALLtR1OJOkpyP9uueklflV_kW7Z9Stq5zFVxWqirHnUryWQtZvvgihVKWltC9d_UoIrVzVPGA7uW90ZfZKPGS7f8hj9oTouxDCOmF37NehA4RQEmYqORCfWl4QRsppLHzugQbgPZwTEp9xiktIkR_PPCNCzFDyNG6SE8Lc5ZJ4ATylQhvS5VPH5-lnQn6_AOWKyoUHPP81poIJBuLLGFeqdInHTLjMF1vKw9JffwjTGPN20VP2qIWe0rM_7w379v726-Fjdff5w6fDu7sqGGFK1WoFMcDRydCKqFoNJhxrbY7WQQNRWSus0UEnF610Kqi2MUaGWkWtjWr3-oa9uPquoe-XRMUPmULqexjTtJBXtXCN0moF7RUMOBFhav2MeVgzein8No-_zOO37r2r_WUe36y6t1ddWlP8yAk9hbXztd6MKRQfp_wfh9_7gJ2A</recordid><startdate>19961001</startdate><enddate>19961001</enddate><creator>Chebotarev, V.V.</creator><creator>Garkusha, I.E.</creator><creator>Garkusha, V.V.</creator><creator>Makhlaj, V.A.</creator><creator>Mitina, N.I.</creator><creator>Solyakov, D.G.</creator><creator>Tereshin, V.I.</creator><creator>Trubchaninov, S.A.</creator><creator>Tsarenko, A.V.</creator><creator>Wuerz, H.</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>19961001</creationdate><title>Characteristics of transient plasma layers produced by irradiation of graphite targets by high power quasi-stationary plasma streams under the disruption simulation conditions</title><author>Chebotarev, V.V. ; Garkusha, I.E. ; Garkusha, V.V. ; Makhlaj, V.A. ; Mitina, N.I. ; Solyakov, D.G. ; Tereshin, V.I. ; Trubchaninov, S.A. ; Tsarenko, A.V. ; Wuerz, H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c404t-f32adcab91cf0d2f3a4cb634b59a7ad2550543c3e9d5192c2f7441c62d3342f83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1996</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chebotarev, V.V.</creatorcontrib><creatorcontrib>Garkusha, I.E.</creatorcontrib><creatorcontrib>Garkusha, V.V.</creatorcontrib><creatorcontrib>Makhlaj, V.A.</creatorcontrib><creatorcontrib>Mitina, N.I.</creatorcontrib><creatorcontrib>Solyakov, D.G.</creatorcontrib><creatorcontrib>Tereshin, V.I.</creatorcontrib><creatorcontrib>Trubchaninov, S.A.</creatorcontrib><creatorcontrib>Tsarenko, A.V.</creatorcontrib><creatorcontrib>Wuerz, H.</creatorcontrib><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of nuclear materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chebotarev, V.V.</au><au>Garkusha, I.E.</au><au>Garkusha, V.V.</au><au>Makhlaj, V.A.</au><au>Mitina, N.I.</au><au>Solyakov, D.G.</au><au>Tereshin, V.I.</au><au>Trubchaninov, S.A.</au><au>Tsarenko, A.V.</au><au>Wuerz, H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Characteristics of transient plasma layers produced by irradiation of graphite targets by high power quasi-stationary plasma streams under the disruption simulation conditions</atitle><jtitle>Journal of nuclear materials</jtitle><date>1996-10-01</date><risdate>1996</risdate><volume>233</volume><issue>1-3</issue><spage>736</spage><epage>740</epage><pages>736-740</pages><issn>0022-3115</issn><eissn>1873-4820</eissn><abstract>Simulation experiments to model the situation occurring at the divertor plates during disruptions and ELMy H-modes of tokamak were carried out with plasma streams generated at the Kharkov QSPA. The facility ultimate plasma parameters were as follows: plasma energy density — above 2 kJ/cm
2, proton energy — 0.9 keV, plasma density — 10
16 cm
−3, pulse duration — 0.1–0.15 ms. Graphite targets of different sizes utilized in these experiments. It was shown that high density target plasma layer, with densities up to 6 · 10
17 cm
−3, were formed above the target surface, when incident plasma interacted with target, and sustained during the whole pulse. Density and thickness (usually within 3 to 5 cm) increased with increasing incident plasma power and target surface. The main part of incident plasma energy (≈ 90%) is absorbed by the transient layer on the first 2–3 cm of its thickness. The average erosion coefficient of the graphite under the influence of incident plasma was of the order of 1 μm/kJ.</abstract><pub>Elsevier B.V</pub><doi>10.1016/S0022-3115(96)00329-7</doi><tpages>5</tpages></addata></record> |
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title | Characteristics of transient plasma layers produced by irradiation of graphite targets by high power quasi-stationary plasma streams under the disruption simulation conditions |
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