{"title":"JET低温泵氮屏蔽热设计优化","authors":"C. Baxi, W. Obert","doi":"10.1109/FUSION.1991.218651","DOIUrl":null,"url":null,"abstract":"Thermal analysis of the nitrogen shield of the JET (Joint European Torus) cryopump was done using a finite element computer program. In this analysis, a parallel flow arrangement and two series flow arrangements were compared for cooldown from 300 to about 80 K. In order to simplify the analysis, coolant was assumed to be a N/sub 2/ gas at an inlet temperature of 80 K. It is shown that all three flow arrangements have similar time for cooling down the shield from 300 to 80 K. This means that the heat exchange effect or radial conduction from the warm part of the shield to the cold part of the shield for series flow arrangements is not dominant. Due to small conduction effects, it will be feasible to modify the design to a more stable series flow arrangement. This flow arrangement will also have minimum cooling time. The inner stainless steel shield has small thermal conductivity and, hence, this part of the shield lags in cooling behind the rest of the shield. This could be remedied by adding about a 1-mm layer of copper in poloidal stripes to the stainless steel fin.<<ETX>>","PeriodicalId":318951,"journal":{"name":"[Proceedings] The 14th IEEE/NPSS Symposium Fusion Engineering","volume":"60 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1991-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Optimization of thermal design for nitrogen shield of JET cryopump\",\"authors\":\"C. Baxi, W. Obert\",\"doi\":\"10.1109/FUSION.1991.218651\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Thermal analysis of the nitrogen shield of the JET (Joint European Torus) cryopump was done using a finite element computer program. In this analysis, a parallel flow arrangement and two series flow arrangements were compared for cooldown from 300 to about 80 K. In order to simplify the analysis, coolant was assumed to be a N/sub 2/ gas at an inlet temperature of 80 K. It is shown that all three flow arrangements have similar time for cooling down the shield from 300 to 80 K. This means that the heat exchange effect or radial conduction from the warm part of the shield to the cold part of the shield for series flow arrangements is not dominant. Due to small conduction effects, it will be feasible to modify the design to a more stable series flow arrangement. This flow arrangement will also have minimum cooling time. The inner stainless steel shield has small thermal conductivity and, hence, this part of the shield lags in cooling behind the rest of the shield. This could be remedied by adding about a 1-mm layer of copper in poloidal stripes to the stainless steel fin.<<ETX>>\",\"PeriodicalId\":318951,\"journal\":{\"name\":\"[Proceedings] The 14th IEEE/NPSS Symposium Fusion Engineering\",\"volume\":\"60 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1991-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"[Proceedings] The 14th IEEE/NPSS Symposium Fusion Engineering\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/FUSION.1991.218651\",\"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.1991.218651","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
利用有限元程序对JET (Joint European Torus)低温泵的氮屏蔽层进行了热分析。在此分析中,比较了平行流动安排和两种串联流动安排的冷却时间从300到大约80 K。为了简化分析,假设冷却剂为入口温度为80k时的N/sub / gas。结果表明,三种流动方式对300 ~ 80k的屏蔽层冷却时间相似。这意味着在串联流动布置中,从护板的温暖部分到护板的寒冷部分的热交换效应或径向传导不占主导地位。由于传导效应小,将设计修改为更稳定的串联流动布置是可行的。这种流动安排也将有最小的冷却时间。内部不锈钢护罩的导热系数很小,因此,这部分护罩的冷却滞后于护罩的其余部分。这可以通过在不锈钢翅片上加一层1毫米厚的极向条纹铜来弥补
Optimization of thermal design for nitrogen shield of JET cryopump
Thermal analysis of the nitrogen shield of the JET (Joint European Torus) cryopump was done using a finite element computer program. In this analysis, a parallel flow arrangement and two series flow arrangements were compared for cooldown from 300 to about 80 K. In order to simplify the analysis, coolant was assumed to be a N/sub 2/ gas at an inlet temperature of 80 K. It is shown that all three flow arrangements have similar time for cooling down the shield from 300 to 80 K. This means that the heat exchange effect or radial conduction from the warm part of the shield to the cold part of the shield for series flow arrangements is not dominant. Due to small conduction effects, it will be feasible to modify the design to a more stable series flow arrangement. This flow arrangement will also have minimum cooling time. The inner stainless steel shield has small thermal conductivity and, hence, this part of the shield lags in cooling behind the rest of the shield. This could be remedied by adding about a 1-mm layer of copper in poloidal stripes to the stainless steel fin.<>