R. Perillo, J. Boedo, C. Lasnier, A. McLean, I. Bykov, C. Marini, D. Rudakov, J. Watkins
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引用次数: 0
摘要
研究发现,携带 1%等离子体存储能量的小型/II 型边缘定位模式(ELM)仅将 45 ± 5% 的 ELM 功率沉积在撞击点附近,其余 55 ± 5% 的功率沉积在远刮擦层(SOL)。与 I 型电致发光器相比,小型电致发光器的功率分布面积更大,在近 SOL 和远 SOL 区域,这一比例分别约为 60% 和 40%。在类似等离子体条件和磁场配置下,小型ELM内部剖面在SOL中的热通量宽度(λq)为6.0毫米,几乎比I型ELM的3.15毫米大2倍。在ELM峰值,小型ELM的λq比I型ELM的λq大4倍,从2毫米到7.9毫米,表明在氖种子小型ELM情况下径向传输增强。在准双空(QDN)放电中,还计算了次级外分流器的 ELM 间 λq。结果发现,与参考的 I 型 ELM 相比,在高分离基质密度的小型 ELM 系统中,λq 平均要大 2.2 倍。用快速往复探头在外侧中平面测量的小型 ELM 径向速度剖面图支持了这些发现,该剖面图显示 SOL 的衰减长度(λvr)为 12.8 厘米,比 I 型 ELM 的 3.9 厘米大 3.3 倍。这一分析表明,虽然小型 ELM 因峰值热通量低和 λq 大而对未来的机器具有吸引力,但可能会因外壁的通量较大而引起关注。
Experimental evidence of enhanced radial transport in small ELM regimes at DIII-D
Small/type-II edge-localized-modes (ELMs), carrying 1% of the plasma stored energy, are found to deposit only 45 ± 5% of the ELM power near the strike point, and the remaining 55 ± 5% to the far scrape-off-layer (SOL). Small ELMs spread their power over a larger area compared to type-I ELMs, where such a ratio is about 60% and 40% for near- and far-SOL regions, respectively. The larger spread is reflected in the heat flux width (λq) in the SOL for the intra-small ELMs profile of 6.0 mm, almost a factor 2 larger than that of type-I ELMs of 3.15 mm, for similar plasma conditions and magnetic configuration. At the ELM peak, the small ELMs λq is found to be up to 4 times larger than for the type-I ELMs, going from 2 to 7.9 mm, indicating enhanced radial transport in the neon-seeded small ELM scenario. Inter-ELM λqs have been also calculated at the secondary outer divertor in quasi-double-null (QDN) discharges. It is found that, on average, λq is 2.2 times larger in the high-separatrix-density small ELM regime, compared to a reference type-I ELM one. These findings are supported by small ELMs radial velocity profiles, measured at the outer midplane with a fast reciprocating probe, showing a decay length (λvr) in the SOL of 12.8 cm, which is 3.3 times larger than that for the type-I ELMs of 3.9 cm. This analysis shows that small ELMs, although attractive for future machines due to low peak heat flux and large λq, might be of concern for the larger flux to the outer wall.