Erosion, transport, and tritium codeposition analysis of a beryllium wall tokamak

被引:9
作者
Brooks, JN
Allain, JP
Alman, DA
Ruzic, DN
机构
[1] Argonne Natl Lab, Argonne, IL 60439 USA
[2] Univ Illinois, Urbana, IL 61801 USA
关键词
tritium codeposition; beryllium; tokamak;
D O I
10.1016/j.fusengdes.2004.10.002
中图分类号
TL [原子能技术]; O571 [原子核物理学];
学科分类号
0827 ; 082701 ;
摘要
We analyzed beryllium first wall sputtering erosion, sputtered material transport, and T/Be codeposition for a typical next-generation tokamak design-the fusion ignition research experiment (FIRE). The results should be broadly applicable to any future tokamak with a beryllium first wall. Starting with a fluid code scrapeoff layer attached plasma solution, plasma D-0 neutral fluxes to the wall and divertor are obtained from the DEGAS2 neutral transport code. The D+ ion flux to the wall is computed using both a diffusive term and a simple convective transport model. Sputtering coefficients for the beryllium wall are given by the VFTRIM-3D binary-collision code. Transport of beryllium to the divertor, plasma, and back to the wall is calculated with the WBC+ code, which tracks sputtered atom ionization and subsequent ion transport along the SOL magnetic field lines. Then, using results from a study of Be/W mixing/sputtering on the divertor, and using REDEP/WBC impurity transport code results, we estimate the divertor surface response. Finally, we compute tritium codeposition rates in Be growth regions on the wall and divertor for D-T plasma shots using surface temperature dependent D-T/Be rates and with different assumed oxygen contents. Key results are: (1) peak wall net erosion rates vary from about 0.3 mm s(-1) for diffusion-only transport to 3 nm s(-1) for diffusion plus convection, (2) T/Be codeposition rates vary from about 0.1 to 10.0 mg T s(-1) depending on the model, and (3) core plasma contamination from wall-sputtered beryllium is low in all cases (< 0.02%). Thus, based on the erosion and codeposition results, the performance of a beryllium first wall is very dependent on the plasma response, and varies from acceptable to unacceptable. (c) 2004 Elsevier B.V. All rights reserved.
引用
收藏
页码:363 / 375
页数:13
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