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Poloidal asymmetries in edge transport barriers

机译:边缘传输势垒中的极向不对称

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Measurements of impurities in Alcator C-Mod indicate that in the pedestal region, significant poloidal asymmetries can exist in the impurity density, ion temperature, and main ion density. In light of the observation that ion temperature and electrostatic potential are not constant on a flux surface [Theiler et al., Nucl. Fusion 54, 083017 (2014)], a technique based on total pressure conservation to align profiles measured at separate poloidal locations is presented and applied. Gyrokinetic neoclassical simulations with XGCa support the observed large poloidal variations in ion temperature and density, and that the total pressure is approximately constant on a flux surface. With the updated alignment technique, the observed in-out asymmetry in impurity density is reduced from previous publishing [Churchill et al., Nucl. Fusion 53, 122002 (2013)], but remains substantial (n(z,H)(z,L) similar to 6). Candidate asymmetry drivers are explored, showing that neither non-uniform impurity sources nor localized fluctuation-driven transport are able to explain satisfactorily the impurity density asymmetry. Since impurity density asymmetries are only present in plasmas with strong electron density gradients, and radial transport timescales become comparable to parallel transport timescales in the pedestal region, it is suggested that global transport effects relating to the strong electron density gradients in the pedestal are the main driver for the pedestal in-out impurity density asymmetry. (C) 2015 AIP Publishing LLC.
机译:Alcator C-Mod中杂质的测量表明,在基座区域,杂质密度,离子温度和主离子密度中可能存在明显的极谱不对称性。根据观察,在通量表面上离子温度和静电势不是恒定的[Theiler et al。,Nucl。 Fusion 54,083017(2014)],一种基于总压力守恒的技术,用于对齐在单独的极点位置处测量的轮廓。用XGCa进行的动力学动力学新古典模拟支持观察到的离子温度和密度的大倍性变化,并且总压力在通量表面上大致恒定。使用更新的对准技术,从先前的出版物中减少了观察到的杂质密度的进出不对称性[Churchill等人,Nucl.Natl.Acad.Sci.USA,89:1877]。 [Fusion 53,122002(2013)],但保持实质性值(n(z,H)/ n(z,L)与6类似)。探索了候选的不对称驱动因素,显示出不均匀的杂质源和局部波动驱动的输运都不能令人满意地解释杂质密度的不对称性。由于杂质密度不对称仅存在于具有强电子密度梯度的等离子体中,并且径向传输时标变得与基座区域中的平行传输时标相当,因此建议与基座中强电子密度梯度有关的整体传输效应是主要的基座进出杂质密度不对称的驱动因素。 (C)2015 AIP Publishing LLC。

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