在热核实验堆基线方案中使用钨和钨等效辐射器 DIII-D 的功率和同位素效应

A. C. C. Sips, Francesca Turco, Charles Mark Greenfield, Lothar Schmitz, Timothy C Luce, Tomas Odstrcil, Adam G McLean, Igor Bykov, A W Hyatt, Tom H Osborne
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摘要

FEC 2023 的贡献:DIII-D 中的实验记录了热核实验堆基线方案(IBS)在 q95 ~ 3 和 PIN/PLH ~ 1-2 条件下,利用 Kr 和 Xe 作为钨等效辐射器在氘和氢中进行的实验。研究发现,H 模式工作(PLH)的功率阈值比比例定律高出约 2 倍。在最近的氘核 IBS 实验中,钨(W)或钼和镍镉等金属的内在含量降低了 20-25%的基座压力。在钨核心浓度 CW = 10-5 时,氘 IBS 等离子体会发生完全辐射坍缩。模拟显示,对于热核实验堆的预期堆芯温度,等离子体在 CW = 1x10-5 时不会发生辐射塌缩,而且在 CW 高达 3x10-5 时仍可达到 Q = 8-10。与氘相比,氢中的 IBS 不受内在高 Z 杂质的影响。在对 IBS 氢放电中的输入功率和杂质流进行矩阵扫描时注入了氪。氢中的氪杂质密度曲线与氘等离子体相似,但在相同输入功率下,Kr流量要高出2-3倍。氪被输送到内核并影响整个半径;在最高注入率下,内核辐射分数为 0.3-0.35 时会发生辐射塌缩,这与预期的 ITER 内核等离子体最大 W 辐射分数一致。将这一结果与之前国际热核聚变实验堆数据库的研究结果进行比较后发现,在高 Z 杂质导致的较高辐射分率下,H98 的下降幅度大于 10%。另一方面,使用 Kr 作为等效 W 辐射体的结果表明,在比 ITER 核心温度更低的情况下,金属(W)设备可能会为 ITER 的氘氚运行提供过于悲观的性能推断。
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Power and isotope effects in the ITER Baseline Scenario with tungsten and tungsten-equivalent radiators in DIII-D
FEC 2023 contribution: Experiments in DIII-D document the ITER Baseline Scenario (IBS) at q95 ~ 3 and PIN/PLH ~ 1-2, in both deuterium and hydrogen utilizing Kr and Xe as Tungsten-equivalent radiators. The power threshold for H-mode operation (PLH) was found to be about a factor of two higher than the scaling law. In recent IBS experiments in deuterium, intrinsic levels of metals such as Tungsten (W) or molybdenum and inconel are present that reduce the pedestal pressure by 20-25%. A complete radiative collapse of deuterium IBS plasmas occurs at W core concentrations CW = 10-5. Simulations show that for core temperatures expected for ITER, the plasmas would not have a radiative collapse at CW = 1x10-5, moreover Q = 8-10 would still be achieved for CW up to 3x10-5. In contrast to deuterium, the IBS in hydrogen is not affected by intrinsic high-Z impurities. Krypton was injected in a matrix scan of input power and impurity flow in IBS hydrogen discharges. Krypton impurity density profiles in hydrogen are similar to deuterium plasmas, but at Kr flows that are 2-3 times higher for the same input power. Krypton is transported into the core and affects the whole radius; at the highest injection rates a radiative collapse occurs at core radiation fractions of 0.3-0.35, consistent with the expected maximum W radiation fraction for ITER core plasmas. Comparing the results with previous ITPA database studies of the IBS confirms that at higher radiation fraction due to high-Z impurities, a drop in H98 of >10% is observed. On the other hand, the results using Kr as a W-equivalent radiator indicate that metal (W) devices at lower core temperatures than ITER may provide overly pessimistic performance extrapolations to ITER for deuterium-tritium operation.
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