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Role Of Elelctrostatic Magnetic Turbulence in ITB Formation In JET

机译:静电和电磁湍流在JET中ITS形成中的作用

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The suppression of edge density turbulence during H-mode phases of tokamak idscharges has long been associate with the formation of an edge transport barrier and a reduction in edge plasma transport. Recent results [1,2] suggest a similar correlation between core turbulence and reduced core transport during optimised or reversed central magnetic shear discharges with an internal Transport Barrier. It is believd that ITBs may be formed through a combination of E*B velocity shear magnetic shear stabilisatio nof plasma turbulence and instabilities [3]. In JET optimised shear discharges [4], results show that the turbulence reduction occurs in two stages. Low frequencies are suppressed throughout the plasma core by a toroidal velocity shear, then high frequencies are locally suppressed around the steep gradient region of the ITB, consistent with E*B poloidal shear.
机译:长期以来,托卡马克电荷的H模式阶段对边缘密度湍流的抑制一直与边缘传输势垒的形成和边缘等离子体传输的减少有关。最近的结果[1,2]表明,在使用内部输运壁垒优化或反向进行的中央磁剪切放电过程中,磁芯湍流与降低的磁芯输运之间具有相似的相关性。人们认为,ITB可能是由E * B速度剪切磁剪切稳定等离子湍流和不稳定性共同形成的[3]。在JET优化的切变排放中[4],结果表明湍流减小发生在两个阶段。环形速度剪切会在整个等离子体核心中抑制低频,然后在ITB的陡峭梯度区域附近局部抑制高频,这与E * B倍体剪切一致。

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