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Turbulence driven widening of the near-SOL power width in ASDEX Upgrade H-Mode discharges

机译:湍流驱动的ASDEX升级H型放电中的近SOL功率宽度变宽

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Divertor heat flux data from infra red (IR) from various tokamaks in H-Mode regime show that the power width, λ_q, scales approximately like 1.6 (R/a)_(ρs,pol). However, the IR based scaling comes with the restriction that only discharges were considered with attached divertor conditions. Here we set up a new data base covering low edge density data but also including high density plasmas reaching the H-mode density limit. We use Thomson-scattering to measure the electron temperature decay length which will set the near-SOL power width through parallel heat conduction. We present scaling results for the density, temperature and pressure separatrix fall-off lengths. As the principal result we derive a generalized power width scaling which reads as λ_q ∝ ρs,pol • (1 + 2.1α_t~(1.7)) where α_t describes a normalized collisionality (α_t = 3 • 10~(-18) Rq~2nZ_(eff)T~(-2)). The parameter α_t describes the relative importance of the interchange effect on drift-wave turbulence as proposed by Scott and is found to be closely linked to the diamagnetic parameter ay introduced by Rogers, Drake and Zeiler (RDZ). The edge operational space for ASDEX Upgrade displays a boundary qualitatively in agreement with the region labelled as density limit in the edge plasma phase space proposed by RDZ. The data base shows in the limit of low edge densities (α_t ≃ 0.2) accurate agreement to the IR based power width scaling. At elevated separatrix densities (α_t ≃ 1) the power width is broadened by a factor of up to about three accompanied by a reduction of the H_(98, y2) confinement factor. Plasmas with higher triangularity show higher values for H_(98, y2) in the same range of normalized collisionality.
机译:来自H模式模式下各种托卡马克的红外(IR)的分流器热通量数据显示,功率宽度λ_q的缩放比例近似为1.6(R / a)_(ρs,pol)。但是,基于IR的缩放带有限制,即只有在附加的分流器条件下才考虑放电。在这里,我们建立了一个新的数据库,该数据库既覆盖低边缘密度数据,又包含达到H模式密度极限的高密度等离子体。我们使用汤姆森散射来测量电子温度的衰减长度,这将通过平行热传导来设定接近SOL的功率宽度。我们提供密度,温度和压力分离线下降长度的缩放结果。作为主要结果,我们得出了广义功率宽度缩放比例,其读数为λ_qρρs,pol•(1 +2.1α_t〜(1.7)),其中α_t描述了规范化的碰撞性(α_t= 3•10〜(-18)Rq〜2nZ_ (eff)T〜(-2))。参数α_t描述了斯科特提出的互换效应对漂移波湍流的相对重要性,并且发现与罗杰斯,德雷克和泽勒(RDZ)引入的抗磁参数ay紧密相关。 ASDEX升级版的边缘操作空间与RDZ提出的边缘等离子体相空间中标记为密度极限的区域在质量上显示了边界。该数据库在低边沿密度(α_t≃0.2)的极限中显示出与基于IR的功率宽度缩放精确一致。在较高的头皮密度(α_t≃1)处,功率宽度最多可扩大至约三倍,同时减小H_(98,y2)限制因子。在相同的归一化碰撞性范围内,具有较高三角形性的等离子体显示出较高的H_(98,y2)值。

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