Tungsten erosion under plasma heat loads typical for ITER type I ELMs and disruptions
The behavior of pure sintered tungsten under repetitive plasma heat loads of ∼1MJ/m2 (which is relevant to ITER ELMs) and 25MJ/m2 (ITER disruptions) is studied with the quasi-steady-state plasma accelerator QSPA Kh-50. The ELM relevant heat loads have resulted in formation of two kinds of crack netw...
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| Veröffentlicht in: | Journal of nuclear materials 2005-03, Vol.337-339, p.707-711 |
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| container_title | Journal of nuclear materials |
| container_volume | 337-339 |
| creator | Garkusha, I.E. Bandura, A.N. Byrka, O.V. Chebotarev, V.V. Landman, I.S. Makhlaj, V.A. Marchenko, A.K. Solyakov, D.G. Tereshin, V.I. Trubchaninov, S.A. Tsarenko, A.V. |
| description | The behavior of pure sintered tungsten under repetitive plasma heat loads of ∼1MJ/m2 (which is relevant to ITER ELMs) and 25MJ/m2 (ITER disruptions) is studied with the quasi-steady-state plasma accelerator QSPA Kh-50. The ELM relevant heat loads have resulted in formation of two kinds of crack networks, with typical sizes of 10–20μm and ∼1mm, at the surface. Tungsten preheating to 600°C indicates that fine intergranular cracks are probably caused by thermal stresses during fast resolidification of the melt, whereas large cracks are the result of ductile-to-brittle transition. For several hundreds of ELM-like exposures, causing surface melting, the melt motion does not dominate the profile of the melt spot. The disruption relevant experiments demonstrated that melt motion became the main factor of tungsten damage. |
| doi_str_mv | 10.1016/j.jnucmat.2004.10.008 |
| format | Article |
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The ELM relevant heat loads have resulted in formation of two kinds of crack networks, with typical sizes of 10–20μm and ∼1mm, at the surface. Tungsten preheating to 600°C indicates that fine intergranular cracks are probably caused by thermal stresses during fast resolidification of the melt, whereas large cracks are the result of ductile-to-brittle transition. For several hundreds of ELM-like exposures, causing surface melting, the melt motion does not dominate the profile of the melt spot. The disruption relevant experiments demonstrated that melt motion became the main factor of tungsten damage.</description><identifier>ISSN: 0022-3115</identifier><identifier>EISSN: 1873-4820</identifier><identifier>DOI: 10.1016/j.jnucmat.2004.10.008</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Disruption ; ELM ; Erosion and deposition ; Surface analysis ; Tungsten</subject><ispartof>Journal of nuclear materials, 2005-03, Vol.337-339, p.707-711</ispartof><rights>2004 Elsevier B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c340t-89b68be0b24ade463e34707163488b98d4701c7699100fca8be21e3047663a643</citedby><cites>FETCH-LOGICAL-c340t-89b68be0b24ade463e34707163488b98d4701c7699100fca8be21e3047663a643</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0022311504007391$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids></links><search><creatorcontrib>Garkusha, I.E.</creatorcontrib><creatorcontrib>Bandura, A.N.</creatorcontrib><creatorcontrib>Byrka, O.V.</creatorcontrib><creatorcontrib>Chebotarev, V.V.</creatorcontrib><creatorcontrib>Landman, I.S.</creatorcontrib><creatorcontrib>Makhlaj, V.A.</creatorcontrib><creatorcontrib>Marchenko, A.K.</creatorcontrib><creatorcontrib>Solyakov, D.G.</creatorcontrib><creatorcontrib>Tereshin, V.I.</creatorcontrib><creatorcontrib>Trubchaninov, S.A.</creatorcontrib><creatorcontrib>Tsarenko, A.V.</creatorcontrib><title>Tungsten erosion under plasma heat loads typical for ITER type I ELMs and disruptions</title><title>Journal of nuclear materials</title><description>The behavior of pure sintered tungsten under repetitive plasma heat loads of ∼1MJ/m2 (which is relevant to ITER ELMs) and 25MJ/m2 (ITER disruptions) is studied with the quasi-steady-state plasma accelerator QSPA Kh-50. The ELM relevant heat loads have resulted in formation of two kinds of crack networks, with typical sizes of 10–20μm and ∼1mm, at the surface. Tungsten preheating to 600°C indicates that fine intergranular cracks are probably caused by thermal stresses during fast resolidification of the melt, whereas large cracks are the result of ductile-to-brittle transition. For several hundreds of ELM-like exposures, causing surface melting, the melt motion does not dominate the profile of the melt spot. The disruption relevant experiments demonstrated that melt motion became the main factor of tungsten damage.</description><subject>Disruption</subject><subject>ELM</subject><subject>Erosion and deposition</subject><subject>Surface analysis</subject><subject>Tungsten</subject><issn>0022-3115</issn><issn>1873-4820</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNqFkFFLwzAUhYMoOKc_QciTb503TZamTyJj6mAiyPYcsvROU7q2Jqmwf2_K9u7T5R7OOXA-Qu4ZzBgw-VjP6nawBxNnOYBI2gxAXZAJUwXPhMrhkkwA8jzjjM2vyU0INQDMS5hPyHYztF8hYkvRd8F1LR3aCj3tGxMOhn6jibTpTBVoPPbOmobuO09Xm-XnKCBd0eX6PVDTVrRywQ99TB3hllztTRPw7nynZPuy3CzesvXH62rxvM4sFxAzVe6k2iHscmEqFJIjFwUUTHKh1K5UVfqYLWRZMoC9NcmbM-QgCim5kYJPycOpt_fdz4Ah6oMLFpvGtNgNQedKlkIURTLOT0abVgaPe917dzD-qBnoEaKu9RmiHiGOcoKYck-nHKYVvw69DtZha7FyHm3UVef-afgDsAl8ig</recordid><startdate>20050301</startdate><enddate>20050301</enddate><creator>Garkusha, I.E.</creator><creator>Bandura, A.N.</creator><creator>Byrka, O.V.</creator><creator>Chebotarev, V.V.</creator><creator>Landman, I.S.</creator><creator>Makhlaj, V.A.</creator><creator>Marchenko, A.K.</creator><creator>Solyakov, D.G.</creator><creator>Tereshin, V.I.</creator><creator>Trubchaninov, S.A.</creator><creator>Tsarenko, A.V.</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20050301</creationdate><title>Tungsten erosion under plasma heat loads typical for ITER type I ELMs and disruptions</title><author>Garkusha, I.E. ; Bandura, A.N. ; Byrka, O.V. ; Chebotarev, V.V. ; Landman, I.S. ; Makhlaj, V.A. ; Marchenko, A.K. ; Solyakov, D.G. ; Tereshin, V.I. ; Trubchaninov, S.A. ; Tsarenko, A.V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c340t-89b68be0b24ade463e34707163488b98d4701c7699100fca8be21e3047663a643</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>Disruption</topic><topic>ELM</topic><topic>Erosion and deposition</topic><topic>Surface analysis</topic><topic>Tungsten</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Garkusha, I.E.</creatorcontrib><creatorcontrib>Bandura, A.N.</creatorcontrib><creatorcontrib>Byrka, O.V.</creatorcontrib><creatorcontrib>Chebotarev, V.V.</creatorcontrib><creatorcontrib>Landman, I.S.</creatorcontrib><creatorcontrib>Makhlaj, V.A.</creatorcontrib><creatorcontrib>Marchenko, A.K.</creatorcontrib><creatorcontrib>Solyakov, D.G.</creatorcontrib><creatorcontrib>Tereshin, V.I.</creatorcontrib><creatorcontrib>Trubchaninov, S.A.</creatorcontrib><creatorcontrib>Tsarenko, A.V.</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of nuclear materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Garkusha, I.E.</au><au>Bandura, A.N.</au><au>Byrka, O.V.</au><au>Chebotarev, V.V.</au><au>Landman, I.S.</au><au>Makhlaj, V.A.</au><au>Marchenko, A.K.</au><au>Solyakov, D.G.</au><au>Tereshin, V.I.</au><au>Trubchaninov, S.A.</au><au>Tsarenko, A.V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Tungsten erosion under plasma heat loads typical for ITER type I ELMs and disruptions</atitle><jtitle>Journal of nuclear materials</jtitle><date>2005-03-01</date><risdate>2005</risdate><volume>337-339</volume><spage>707</spage><epage>711</epage><pages>707-711</pages><issn>0022-3115</issn><eissn>1873-4820</eissn><abstract>The behavior of pure sintered tungsten under repetitive plasma heat loads of ∼1MJ/m2 (which is relevant to ITER ELMs) and 25MJ/m2 (ITER disruptions) is studied with the quasi-steady-state plasma accelerator QSPA Kh-50. The ELM relevant heat loads have resulted in formation of two kinds of crack networks, with typical sizes of 10–20μm and ∼1mm, at the surface. Tungsten preheating to 600°C indicates that fine intergranular cracks are probably caused by thermal stresses during fast resolidification of the melt, whereas large cracks are the result of ductile-to-brittle transition. For several hundreds of ELM-like exposures, causing surface melting, the melt motion does not dominate the profile of the melt spot. The disruption relevant experiments demonstrated that melt motion became the main factor of tungsten damage.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.jnucmat.2004.10.008</doi><tpages>5</tpages></addata></record> |
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| subjects | Disruption ELM Erosion and deposition Surface analysis Tungsten |
| title | Tungsten erosion under plasma heat loads typical for ITER type I ELMs and disruptions |
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