{"title":"用于托卡马克等离子体启动模拟的钨壁溅射模型","authors":"Sangil Lee, Jeongwon Lee, Jaemin Kwon","doi":"10.1088/1361-6587/ad6a87","DOIUrl":null,"url":null,"abstract":"Tungsten (W) is the most probable material for the plasma-facing components of fusion reactors due to its excellent thermal and physical properties. A W-wall sputtering model has been established to simulate the start-up of a tokamak plasma using the 0D simulation code DYON. This model incorporates the revised Bohdansky formula to calculate the sputtering yield and a modified formula for calculating the energy impacting the walls. This formula integrates the temporal behavior of electron and ion temperatures at the plasma edge, which has been partially verified by the Thomson scattering diagnostic data. With the new model in place, predictive simulations were conducted for KSTAR’s Ohmic plasma under two W-wall scenarios: one with the entire wall surface covered by W and the other with 95% coverage of W and 5% coverage of carbon (C). The results indicate that the full-W wall may perform better from the perspective of start-up performance. The disparity can primarily be attributed to impurities generated through sputtering and recycling on the C wall. The validity of this model will be finally confirmed when the Thomson diagnostic system is able to precisely measure the edge electron temperature during plasma start-up.","PeriodicalId":20239,"journal":{"name":"Plasma Physics and Controlled Fusion","volume":"1 1","pages":""},"PeriodicalIF":2.1000,"publicationDate":"2024-08-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A tungsten-wall sputtering model for the plasma start-up simulation in tokamaks\",\"authors\":\"Sangil Lee, Jeongwon Lee, Jaemin Kwon\",\"doi\":\"10.1088/1361-6587/ad6a87\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Tungsten (W) is the most probable material for the plasma-facing components of fusion reactors due to its excellent thermal and physical properties. A W-wall sputtering model has been established to simulate the start-up of a tokamak plasma using the 0D simulation code DYON. This model incorporates the revised Bohdansky formula to calculate the sputtering yield and a modified formula for calculating the energy impacting the walls. This formula integrates the temporal behavior of electron and ion temperatures at the plasma edge, which has been partially verified by the Thomson scattering diagnostic data. With the new model in place, predictive simulations were conducted for KSTAR’s Ohmic plasma under two W-wall scenarios: one with the entire wall surface covered by W and the other with 95% coverage of W and 5% coverage of carbon (C). The results indicate that the full-W wall may perform better from the perspective of start-up performance. The disparity can primarily be attributed to impurities generated through sputtering and recycling on the C wall. The validity of this model will be finally confirmed when the Thomson diagnostic system is able to precisely measure the edge electron temperature during plasma start-up.\",\"PeriodicalId\":20239,\"journal\":{\"name\":\"Plasma Physics and Controlled Fusion\",\"volume\":\"1 1\",\"pages\":\"\"},\"PeriodicalIF\":2.1000,\"publicationDate\":\"2024-08-13\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Plasma Physics and Controlled Fusion\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-6587/ad6a87\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, FLUIDS & PLASMAS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Physics and Controlled Fusion","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-6587/ad6a87","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
引用次数: 0
摘要
钨(W)因其优异的热性能和物理性能,最有可能成为聚变反应堆面向等离子体部件的材料。利用 0D 模拟代码 DYON 建立了一个 W 壁溅射模型,用于模拟托卡马克等离子体的启动。该模型采用了经修订的博丹斯基公式来计算溅射产率,并采用了经修订的公式来计算撞击壁面的能量。该公式综合了等离子体边缘电子和离子温度的时间行为,并通过汤姆逊散射诊断数据进行了部分验证。有了这个新模型,我们对 KSTAR 的欧姆等离子体进行了两种 W 壁情况下的预测模拟:一种是整个壁面都被 W 覆盖,另一种是 95% 的 W 和 5% 的碳(C)覆盖。结果表明,从启动性能的角度来看,全 W 壁的性能可能更好。这种差异主要是由于在 C 壁上通过溅射和回收产生的杂质造成的。当汤姆逊诊断系统能够精确测量等离子体启动过程中的边缘电子温度时,这一模型的有效性将得到最终证实。
A tungsten-wall sputtering model for the plasma start-up simulation in tokamaks
Tungsten (W) is the most probable material for the plasma-facing components of fusion reactors due to its excellent thermal and physical properties. A W-wall sputtering model has been established to simulate the start-up of a tokamak plasma using the 0D simulation code DYON. This model incorporates the revised Bohdansky formula to calculate the sputtering yield and a modified formula for calculating the energy impacting the walls. This formula integrates the temporal behavior of electron and ion temperatures at the plasma edge, which has been partially verified by the Thomson scattering diagnostic data. With the new model in place, predictive simulations were conducted for KSTAR’s Ohmic plasma under two W-wall scenarios: one with the entire wall surface covered by W and the other with 95% coverage of W and 5% coverage of carbon (C). The results indicate that the full-W wall may perform better from the perspective of start-up performance. The disparity can primarily be attributed to impurities generated through sputtering and recycling on the C wall. The validity of this model will be finally confirmed when the Thomson diagnostic system is able to precisely measure the edge electron temperature during plasma start-up.
期刊介绍:
Plasma Physics and Controlled Fusion covers all aspects of the physics of hot, highly ionised plasmas. This includes results of current experimental and theoretical research on all aspects of the physics of high-temperature plasmas and of controlled nuclear fusion, including the basic phenomena in highly-ionised gases in the laboratory, in the ionosphere and in space, in magnetic-confinement and inertial-confinement fusion as well as related diagnostic methods.
Papers with a technological emphasis, for example in such topics as plasma control, fusion technology and diagnostics, are welcomed when the plasma physics is an integral part of the paper or when the technology is unique to plasma applications or new to the field of plasma physics. Papers on dusty plasma physics are welcome when there is a clear relevance to fusion.