Evaluation of local erosion and deposition on the W-monoblock of JA-DEMO divertor

IF 2.3 2区 物理与天体物理 Q1 NUCLEAR SCIENCE & TECHNOLOGY
M. Oya , K. Hoshino , N. Asakura , Y. Sakamoto , N. Ohno , K. Hanada
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Abstract

We developed and performed a 3D Monte-Carlo simulation on local erosion and deposition in outer divertor target of JA-DEMO. The local erosion and deposition were evaluated considering the divertor plasma parameters and the roof shape of W-monoblocks. First, for local erosion simulation, the trajectories of D ions and impurity (He and Ar) ions were traced before irradiating the monoblock surface. The physical sputtering was calculated by these ions irradiation, considering their charge states, incident-energies and -angles. The highest sputtering flux was produced by multiply-charged Ar ions (Ar3+–Ar5+). The sputtering flux strongly depended on the poloidal positions along the divertor target. Although almost no erosion (sputtering) was obtained in low-temperature zone (∼1 eV), the erosion occurred in mid- (∼10 eV) and high-temperature (>10 eV) zone. Second, for local deposition simulation, the trajectories of W atoms emitted from the monoblock surface were traced. After transport (including ionization and recombination) in the plasma, W atoms and ions were deposited on the monoblock surface. The deposition occurred even on the area where plasmas did not irradiate (shadow). This was due to perpendicular diffusion to magnetic field lines, gyro-orbit effects for W ions and straight-line motion for neutral W atoms. The poloidal distribution of the deposition fluxes was similar to that of the sputtering fluxes. In low-temperature zone, no deposition flux occurred due to very low sputtering flux. The deposition flux in mid-temperature zone increased significantly and that in high-temperature zone remained high.
评估 JA-DEMO 分流 W 单体的局部侵蚀和沉积情况
我们开发并进行了 JA-DEMO 外岔道靶局部侵蚀和沉积的三维蒙特卡洛模拟。考虑到辐照器等离子体参数和 W 单块的顶盖形状,我们对局部侵蚀和沉积进行了评估。首先,为了进行局部侵蚀模拟,在辐照单块表面之前跟踪了 D 离子和杂质(He 和 Ar)离子的轨迹。考虑到这些离子的电荷状态、入射能量和角度,通过这些离子的辐照计算出物理溅射。多电荷氩离子(Ar3+-Ar5+)产生的溅射通量最高。溅射通量在很大程度上取决于沿分流靶的极性位置。虽然在低温区(∼1 eV)几乎没有侵蚀(溅射),但在中温(∼10 eV)和高温(>10 eV)区出现了侵蚀。其次,为了进行局部沉积模拟,对从单块表面发射的 W 原子的轨迹进行了追踪。在等离子体中传输(包括电离和重组)后,W 原子和离子沉积在单体表面。沉积甚至发生在等离子体未照射的区域(阴影)。这是由于垂直于磁场线的扩散、W 离子的陀螺轨道效应和中性 W 原子的直线运动。沉积通量的极性分布与溅射通量相似。在低温区,由于溅射通量非常低,因此没有沉积通量。中温区的沉积通量显著增加,而高温区的沉积通量仍然很高。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Nuclear Materials and Energy
Nuclear Materials and Energy Materials Science-Materials Science (miscellaneous)
CiteScore
3.70
自引率
15.40%
发文量
175
审稿时长
20 weeks
期刊介绍: The open-access journal Nuclear Materials and Energy is devoted to the growing field of research for material application in the production of nuclear energy. Nuclear Materials and Energy publishes original research articles of up to 6 pages in length.
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