Characteristics of melt convection during Kyropoulos sapphire crystal growth
Melt flows in the Kyropoulos sapphire growth system include Marangoni convection and buoyancy convection. From the seeding stage to the final growth stage, both the area of the free surface and melt height decrease to zero from initial values, and hence the flow pattern in the melt varies during gro...
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Veröffentlicht in: | International journal of materials research 2014-10, Vol.105 (10), p.961-967 |
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description | Melt flows in the Kyropoulos sapphire growth system include Marangoni convection and buoyancy convection. From the seeding stage to the final growth stage, both the area of the free surface and melt height decrease to zero from initial values, and hence the flow pattern in the melt varies during growth. To study systematically melt convection and its influence on the growth process, a non-dimensional parameter is introduced to denote the relative strength of Marangoni convection to buoyancy convection. Temperature and stream function distributions for the different growth stages are simulated. It is found that Marangoni convection is negligible during the early growth. However, it plays an important role in the late growth. The remelting of the crystal surface starts when Marangoni convection becomes dominant, and thus it may be related to this convection mode. The interface shape is found to be changing during the whole growth process, which reduces the industrial productivity of sapphire. Interface convexity, crystal diameter and the non-dimensional parameter are presented as functions of the melt height. Interface convexity is further described as a function of the non-dimensional parameter. The results are consistent with experimentally observed phenomena. |
doi_str_mv | 10.3139/146.111107 |
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From the seeding stage to the final growth stage, both the area of the free surface and melt height decrease to zero from initial values, and hence the flow pattern in the melt varies during growth. To study systematically melt convection and its influence on the growth process, a non-dimensional parameter is introduced to denote the relative strength of Marangoni convection to buoyancy convection. Temperature and stream function distributions for the different growth stages are simulated. It is found that Marangoni convection is negligible during the early growth. However, it plays an important role in the late growth. The remelting of the crystal surface starts when Marangoni convection becomes dominant, and thus it may be related to this convection mode. The interface shape is found to be changing during the whole growth process, which reduces the industrial productivity of sapphire. Interface convexity, crystal diameter and the non-dimensional parameter are presented as functions of the melt height. Interface convexity is further described as a function of the non-dimensional parameter. The results are consistent with experimentally observed phenomena.</description><identifier>ISSN: 1862-5282</identifier><identifier>EISSN: 2195-8556</identifier><identifier>DOI: 10.3139/146.111107</identifier><language>eng</language><publisher>De Gruyter</publisher><subject>Buoyancy ; Computer simulation ; Convection ; Convexity ; Growth from melt ; Industrial crystallization ; Marangoni convection ; Melts ; Melts (crystal growth) ; Nucleation ; Productivity ; Sapphire</subject><ispartof>International journal of materials research, 2014-10, Vol.105 (10), p.961-967</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c307t-4d73accab8dceb0788720009f37728ee5a6a1668396e7ae72f45a5efe707f4dc3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.degruyter.com/document/doi/10.3139/146.111107/pdf$$EPDF$$P50$$Gwalterdegruyter$$H</linktopdf><linktohtml>$$Uhttps://www.degruyter.com/document/doi/10.3139/146.111107/html$$EHTML$$P50$$Gwalterdegruyter$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,66754,68538</link.rule.ids></links><search><creatorcontrib>Fang, HaiSheng</creatorcontrib><creatorcontrib>Zhang, Zhi</creatorcontrib><creatorcontrib>Jin, ZeLin</creatorcontrib><creatorcontrib>Wang, Sen</creatorcontrib><creatorcontrib>Xu, JianFeng</creatorcontrib><title>Characteristics of melt convection during Kyropoulos sapphire crystal growth</title><title>International journal of materials research</title><description>Melt flows in the Kyropoulos sapphire growth system include Marangoni convection and buoyancy convection. From the seeding stage to the final growth stage, both the area of the free surface and melt height decrease to zero from initial values, and hence the flow pattern in the melt varies during growth. To study systematically melt convection and its influence on the growth process, a non-dimensional parameter is introduced to denote the relative strength of Marangoni convection to buoyancy convection. Temperature and stream function distributions for the different growth stages are simulated. It is found that Marangoni convection is negligible during the early growth. However, it plays an important role in the late growth. The remelting of the crystal surface starts when Marangoni convection becomes dominant, and thus it may be related to this convection mode. The interface shape is found to be changing during the whole growth process, which reduces the industrial productivity of sapphire. Interface convexity, crystal diameter and the non-dimensional parameter are presented as functions of the melt height. Interface convexity is further described as a function of the non-dimensional parameter. The results are consistent with experimentally observed phenomena.</description><subject>Buoyancy</subject><subject>Computer simulation</subject><subject>Convection</subject><subject>Convexity</subject><subject>Growth from melt</subject><subject>Industrial crystallization</subject><subject>Marangoni convection</subject><subject>Melts</subject><subject>Melts (crystal growth)</subject><subject>Nucleation</subject><subject>Productivity</subject><subject>Sapphire</subject><issn>1862-5282</issn><issn>2195-8556</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNqFkMtOwzAQRS0EEuWx4Qu8REgpfsSPsEMVL1GJDawt15m0qdI42A5V_h6jskRiNjOLM1e6B6ErSuac8uqWlnJO8xB1hGaMVqLQQshjNKNaskIwzU7RWYxbQgSVis3QcrGxwboEoY2pdRH7Bu-gS9j5_gtcan2P6zG0_Rq_TsEPfux8xNEOw6YNgF2YYrIdXge_T5sLdNLYLsLl7z5HH48P74vnYvn29LK4XxaOE5WKslbcOmdXunawIkprxQghVcOVYhpAWGmplJpXEpQFxZpSWAENKKKasnb8HF0fcofgP0eIyeza6KDrbA9-jIYqIogUXFb_o1ILTZguWUZvDqgLPsYAjRlCu7NhMpSYH7sm2zUHuxm-O8B722V5NazDOOXDbP0Y-lz-jyeapZNKUv4NqMx_Og</recordid><startdate>20141001</startdate><enddate>20141001</enddate><creator>Fang, HaiSheng</creator><creator>Zhang, Zhi</creator><creator>Jin, ZeLin</creator><creator>Wang, Sen</creator><creator>Xu, JianFeng</creator><general>De Gruyter</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QF</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>7QH</scope><scope>7UA</scope><scope>C1K</scope><scope>F1W</scope><scope>H96</scope><scope>L.G</scope></search><sort><creationdate>20141001</creationdate><title>Characteristics of melt convection during Kyropoulos sapphire crystal growth</title><author>Fang, HaiSheng ; Zhang, Zhi ; Jin, ZeLin ; Wang, Sen ; Xu, JianFeng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c307t-4d73accab8dceb0788720009f37728ee5a6a1668396e7ae72f45a5efe707f4dc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Buoyancy</topic><topic>Computer simulation</topic><topic>Convection</topic><topic>Convexity</topic><topic>Growth from melt</topic><topic>Industrial crystallization</topic><topic>Marangoni convection</topic><topic>Melts</topic><topic>Melts (crystal growth)</topic><topic>Nucleation</topic><topic>Productivity</topic><topic>Sapphire</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Fang, HaiSheng</creatorcontrib><creatorcontrib>Zhang, Zhi</creatorcontrib><creatorcontrib>Jin, ZeLin</creatorcontrib><creatorcontrib>Wang, Sen</creatorcontrib><creatorcontrib>Xu, JianFeng</creatorcontrib><collection>CrossRef</collection><collection>Aluminium Industry Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Aqualine</collection><collection>Water Resources Abstracts</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><jtitle>International journal of materials research</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fang, HaiSheng</au><au>Zhang, Zhi</au><au>Jin, ZeLin</au><au>Wang, Sen</au><au>Xu, JianFeng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Characteristics of melt convection during Kyropoulos sapphire crystal growth</atitle><jtitle>International journal of materials research</jtitle><date>2014-10-01</date><risdate>2014</risdate><volume>105</volume><issue>10</issue><spage>961</spage><epage>967</epage><pages>961-967</pages><issn>1862-5282</issn><eissn>2195-8556</eissn><abstract>Melt flows in the Kyropoulos sapphire growth system include Marangoni convection and buoyancy convection. From the seeding stage to the final growth stage, both the area of the free surface and melt height decrease to zero from initial values, and hence the flow pattern in the melt varies during growth. To study systematically melt convection and its influence on the growth process, a non-dimensional parameter is introduced to denote the relative strength of Marangoni convection to buoyancy convection. Temperature and stream function distributions for the different growth stages are simulated. It is found that Marangoni convection is negligible during the early growth. However, it plays an important role in the late growth. The remelting of the crystal surface starts when Marangoni convection becomes dominant, and thus it may be related to this convection mode. The interface shape is found to be changing during the whole growth process, which reduces the industrial productivity of sapphire. Interface convexity, crystal diameter and the non-dimensional parameter are presented as functions of the melt height. Interface convexity is further described as a function of the non-dimensional parameter. The results are consistent with experimentally observed phenomena.</abstract><pub>De Gruyter</pub><doi>10.3139/146.111107</doi><tpages>7</tpages></addata></record> |
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subjects | Buoyancy Computer simulation Convection Convexity Growth from melt Industrial crystallization Marangoni convection Melts Melts (crystal growth) Nucleation Productivity Sapphire |
title | Characteristics of melt convection during Kyropoulos sapphire crystal growth |
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