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A simulation study of large power handling in the divertor for a Demo reactor

机译:演示反应堆分流器中大功率处理的仿真研究

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摘要

Power exhaust for a 3 GW class fusion reactor with an ITER-sized plasma was investigated by enhancing the radiation loss from seeding impurity. The impurity transport and plasma detachment were simulated under the Demo divertor condition using an integrated divertor code SONIC, in which the impurity Monte-Carlo code, IMPMC, can handle most kinetic effects on the impurity ions in the original formula. The simulation results of impurity species from low Z (neon) to high Z (krypton) and divertor length with a plasma exhausted power of 500 MW and radiation loss of 460 MW, and a fixed core-edge boundary of 7 × 10~(19) m~(-3) were investigated at the first stage for the Demo divertor operation scenario and the geometry design. Results for the different seeding impurities showed that the total heat load, including the plasma transport (q_(target)~(plasma) and radiation (q_(target)~(rad)) was reduced from 15-16 MWm~(-2) (Ne and Ar) to 11 MW m~(-2) for the higher Z (Kr), and q_(target)~(rad) extended over a wide area accompanied by increasing impurity recycling. The geometry effect of the long-leg divertor showed that full detachment was obtained, and the peak q_(target) value was decreased to 12MWm~(-2), where neutral heat load became comparable to q_(target)~(plasma)and q_(target)~(rad)due to smaller flux expansion. Fuel dilution was reduced but was still at a high level. These results showed that a divertor design with a long leg with higher Z seeding such as Ar and Kr is not fulfilled, but will be appropriate to obtain the divertor scenario for the Demo divertor. Finally, influences of χ and D_⊥ enhancement were seen significantly in the divertor, i.e. the radiation and density profiles became wider, leading to full detachment. Both ^target near the separatrix and T_e at the outer flux surfaces were decreased to a level for the conventional technology design. On the other hand, the problem of fuel dilution became worse. Extrapolation of the plasma transport coefficients to ITER and Demo, where density and temperature will be higher than ITER and edge-localized modes are mitigated, is a key issue for the divertor design.
机译:通过增加晶种杂质的辐射损耗,研究了具有ITER尺寸等离子体的3 GW级聚变反应堆的动力排气。使用集成的分流器代码SONIC在Demo分离器条件下模拟了杂质的传输和等离子体的分离,其中杂质蒙特卡罗代码IMPMC可以处理原始公式中对杂质离子的大部分动力学影响。从低Z(氖)到高Z(k)和偏滤器长度的杂质种类的模拟结果,其等离子耗尽功率为500 MW,辐射损耗为4​​60 MW,且核心边缘边界固定为7×10〜(19在第一阶段研究了m〜(-3)的演示偏滤器操作方案和几何设计。不同种子杂质的结果表明,包括等离子体传输(q_(target)〜(plasma)和辐射(q_(target)〜(rad))在内的总热负荷从15-16 MWm〜(-2)降低。 Z(Kr)较高时,从(Ne和Ar)到11 MW m〜(-2),q_(目标)〜(rad)扩展到一个较大的区域,伴随着杂质再循环的增加。偏滤器显示获得了完全脱离,并且q_(目标)的峰值降低到12MWm〜(-2),其中中性热负荷变得与q_(目标)〜(等离子体)和q_(目标)〜(rad)相当。由于通量膨胀较小,降低了燃料稀释度,但仍处于较高水平,这些结果表明,不能满足长支腿且Z籽晶含量较高(例如Ar和Kr)的分流器设计,但适合于获得分流器最后,在偏滤器中可见到χ和D_⊥增强的影响,即辐射和密度分布变宽,导致g完全脱离。在分离线附近的目标和在外部通量表面的T_e都减小到常规技术设计的水平。另一方面,燃料稀释的问题变得更加严重。等离子体传输系数外推至ITER和Demo,密度和温度将高于ITER,并且减轻了边缘局限模式,这是分流器设计的关键问题。

著录项

  • 来源
    《Nuclear fusion》 |2013年第12期|123013.1-123013.15|共15页
  • 作者单位

    Japan Atomic Energy Agency, Rokkasho, Aomori 039-3212, Japan;

    Japan Atomic Energy Agency, Naka, Ibaraki 311-0193, Japan;

    Japan Atomic Energy Agency, Rokkasho, Aomori 039-3212, Japan;

    Japan Atomic Energy Agency, Rokkasho, Aomori 039-3212, Japan;

    Japan Atomic Energy Agency, Rokkasho, Aomori 039-3212, Japan;

    Osaka University, Graduate School of Engineering, Suita, Osaka 565-0871, Japan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
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