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Formation, sustainment and characteristics of current hole plasmas in DIII-D discharges

机译:DIII-D放电中电流空穴等离子体的形成,维持和特性

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Plasmas with zero or near-zero current density in a wide region of the core have been produced in DIII-D discharges. The discharges were obtained with early neutral beam and electron cyclotron heating (ECH) during the plasma current ramp. Wide current holes (CHs) with a near-zero field over about 23% of the plasma width and narrow CHs with a duration of up to 1.1s (comparable to the current relaxation time) have been obtained. Equilibria and pressure profiles were obtained by including kinetic and motional Stark effect (MSE) data using the code TRANSP. Agreement between calculated and measured neutron fluxes is obtained only when the fast-ion diffusion coefficient is set to very high values which results in considerable fast-ion redistribution and a broadened pressure profile. The MSE-only equilibrium fits are in good agreement with such kinetic fits. While CHs collapse due to tearing modes, bursty MHD activity coherent with electron temperature relaxation events is observed when the CHs are sustained. Some collapse events also appear to be coincident with edge localized modes. The CH phase seems to have been limited by the no-wall beta limit. In the present set of discharges, wider CHs (steeper temperature gradients) appear to collapse at somewhat lower β. Tearing modes are seen to cause shrinking of the CH. While early electron heating is strongly dependent on the timing and power of the neutral beam and by the ECH power, it is seen that larger neutral beam powers are correlated with wider CHs which do not decay significantly. An extensive and perhaps difficult analysis of current transport is required to check whether a neoclassical poloidal flux evolution (diffusive EMF) is either consistent with a stationary current profile or that an additional or anomalous EMF is present.
机译:在DIII-D放电中,在铁芯的较宽区域产生了电流密度为零或接近零的等离子体。在等离子体电流斜坡期间,通过早期中性束和电子回旋加速器加热(ECH)获得了放电。已获得在等离子宽度约23%处具有接近零场的宽电流孔(CH)和持续时间长达1.1s(与电流弛豫时间相比)的窄CHs。通过使用代码TRANSP包括动力学和运动Stark效应(MSE)数据来获得平衡和压力曲线。仅当快速离子扩散系数设置为非常高的值时,才能获得计算出的中子通量和测量到的中子通量之间的一致性,这会导致大量的快速离子重新分布并扩大压力分布。仅MSE的平衡拟合与这种动力学拟合非常吻合。当CHs由于撕裂模式而崩溃时,当CHs维持时,观察到与电子温度弛豫事件相一致的爆发性MHD活性。一些倒塌事件似乎也与边缘局部化模式一致。 CH阶段似乎受到无壁β限制的限制。在当前的一组放电中,较宽的CHs(较陡的温度梯度)似乎在较低的β处塌陷。撕裂模式被认为会导致CH的收缩。尽管早期电子加热在很大程度上取决于中性束的时间和功率以及ECH功率,但可以看出,较大的中性束功率与较宽的CH相关,而CH不会明显衰减。需要对电流传输进行广泛且可能困难的分析,以检查新古典的极谱通量演化(扩散性EMF)是否与静态电流曲线一致,或者是否存在额外的或异常的EMF。

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