{"title":"CFD代码中粒子再悬浮模型的实现:在真空环形容器空气进入场景中的应用","authors":"T. Gelain, L. Ricciardi, F. Gensdarmes","doi":"10.1115/icone2020-16139","DOIUrl":null,"url":null,"abstract":"\n During a loss of vacuum accident (LOVA), dust particles that will be present in the future tokamak ITER are likely to be resuspended, inducing a risk for explosion and airborne contamination. Evaluating the particle resuspension/deposition and resulting airborne concentration in case of a LOVA is therefore a major issue and it can be investigated by using a CFD code. To this end, this article presents the implementation of a resuspension model in a CFD code (ANSYS CFX) and its application to an air ingress in a vacuum toroidal vessel with a volume comparable to ITER one.\n In the first part of the article, the Rock’n Roll model and its operational version with the Biasi’s correlation is presented.\n The second part of the article will be devoted to the implementation of the Rock’n’Roll model in ANSYS CFX for constant friction velocities and its adaptation to non-constant friction velocities.\n Finally, the paper presents the simulations obtained on the particle resuspension for an air ingress scenario in a large vacuum vessel. This case is particularly interesting and non-intuitive because as the initial pressure is reduced, the particle behavior is different from that at atmospheric pressure. Further, a competition between airflow forces and gravitational force occurs, due to the low pressure environment, potentially restricting the resuspension, and the pressure influence also has to be taken into account in the particle transport and deposition (Nerisson, 2011).\n Three particle diameters were studied allowing to show the evolution of the resuspension with this parameter and to calculate dust resuspension rates and airborne fractions during the air ingress.","PeriodicalId":63646,"journal":{"name":"核工程研究与设计","volume":"68 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2020-08-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Implementation of a Particle Resuspension Model in a CFD Code: Application to an Air Ingress Scenario in a Vacuum Toroidal Vessel\",\"authors\":\"T. Gelain, L. Ricciardi, F. 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引用次数: 0
摘要
在失去真空事故(LOVA)期间,未来托卡马克ITER中存在的粉尘颗粒可能会重新悬浮,从而引发爆炸和空气污染的风险。因此,在LOVA的情况下,评估颗粒的再悬浮/沉积以及由此产生的空气中浓度是一个主要问题,可以通过使用CFD代码进行研究。为此,本文提出了在CFD代码(ANSYS CFX)中实现重悬浮模型,并将其应用于容积与ITER相当的真空环形容器的进气口。在文章的第一部分,Rock 'n Roll模型及其与Biasi相关的操作版本被提出。文章的第二部分将致力于在ANSYS CFX中实现恒摩擦速度的Rock 'n 'Roll模型及其对非恒摩擦速度的适应。最后,本文给出了大型真空容器空气进入情况下粒子再悬浮的模拟结果。这种情况特别有趣,也不直观,因为当初始压力降低时,粒子的行为与大气压下的不同。此外,由于低压环境,气流力和重力之间的竞争可能会限制再悬浮,并且在颗粒的运输和沉积中也必须考虑压力的影响(Nerisson, 2011)。研究了三种颗粒直径,允许用该参数显示再悬浮的演变,并计算了空气进入过程中的粉尘再悬浮率和空气中的分数。
Implementation of a Particle Resuspension Model in a CFD Code: Application to an Air Ingress Scenario in a Vacuum Toroidal Vessel
During a loss of vacuum accident (LOVA), dust particles that will be present in the future tokamak ITER are likely to be resuspended, inducing a risk for explosion and airborne contamination. Evaluating the particle resuspension/deposition and resulting airborne concentration in case of a LOVA is therefore a major issue and it can be investigated by using a CFD code. To this end, this article presents the implementation of a resuspension model in a CFD code (ANSYS CFX) and its application to an air ingress in a vacuum toroidal vessel with a volume comparable to ITER one.
In the first part of the article, the Rock’n Roll model and its operational version with the Biasi’s correlation is presented.
The second part of the article will be devoted to the implementation of the Rock’n’Roll model in ANSYS CFX for constant friction velocities and its adaptation to non-constant friction velocities.
Finally, the paper presents the simulations obtained on the particle resuspension for an air ingress scenario in a large vacuum vessel. This case is particularly interesting and non-intuitive because as the initial pressure is reduced, the particle behavior is different from that at atmospheric pressure. Further, a competition between airflow forces and gravitational force occurs, due to the low pressure environment, potentially restricting the resuspension, and the pressure influence also has to be taken into account in the particle transport and deposition (Nerisson, 2011).
Three particle diameters were studied allowing to show the evolution of the resuspension with this parameter and to calculate dust resuspension rates and airborne fractions during the air ingress.