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Requirements on localized current drive for the suppression of neoclassical tearing modes

机译:抑制新古典撕裂模式的局部电流驱动要求

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摘要

A heuristic criterion for the full suppression of an NTM was formulated as η_(ntm) ≡ j_(cd,max)/J_(bs) ≥1-2 (Zohm et al 2005 J. Phys. Conf. Ser. 25 234), where j_(cd.max) is the maximum in the driven current density profile applied to stabilize the mode and j_(bs) is the local bootstrap current density. In this work we subject this criterion to a systematic theoretical analysis on the basis of the generalized Rutherford equation. Taking into account only the effect of j_(cd) inside the island, a new criterion for full suppression by a minimum applied total current is obtained in the form of a maximum allowed value for the width of the driven current, w_(dep), combined with a required minimum for the total driven current in the form of w_(dep)η_(ntm) where both limits depend on the marginal and saturated island sizes. These requirements can be relaxed when additional effects are taken into account, such as a change in the stability parameter △' from the current driven outside the island, power modulation, the accompanying heating inside the island or when the current drive is applied preemptively. When applied to ITER scenario 2, the requirement for full suppression of either the 3/2 or 2/1 NTM becomes w_(dep) < 5 cm and w_(dep)η_(ntm) > 5 cm in agreement with (Sauter et al 2010 Plasma Phys. Control. Fusion 52 025002). Optimization of the ITER ECRH Upper Port Launcher design towards minimum required power for full NTM suppression requires an increase in the toroidal injection angle of the lower steering mirror of several degrees compared with its present design value, while for the upper steering mirror the present design value is close to the optimum.
机译:完全抑制NTM的启发式标准公式为η_(ntm)≡j_(cd,max)/ J_(bs)≥1-2(Zohm等,2005 J. Phys。Conf。Ser。25 234),其中j_(cd.max)是为稳定模式而应用的驱动电流密度曲线中的最大值,而j_(bs)是局部自举电流密度。在这项工作中,我们基于广义的卢瑟福方程对该准则进行了系统的理论分析。仅考虑岛内j_(cd)的影响,就可以以驱动电流宽度w_(dep)的最大允许值的形式获得通过最小施加的总电流进行完全抑制的新标准,结合以w_(dep)η_(ntm)形式表示的总驱动电流的最小值,其中两个限制都取决于边缘和饱和岛的大小。当考虑到其他影响时,可以放宽这些要求,例如,由孤岛外部驱动的电流引起的稳定性参数△'的变化,功率调制,孤岛内部伴随的发热或抢先应用电流驱动时。当应用于ITER场景2时,完全抑制3/2或2/1 NTM的要求变为w_(dep)<5 cm和w_(dep)η_(ntm)> 5 cm,这与(Sauter等人2010 Plasma Phys.Control.Fusion 52 025002)。针对ITER ECRH上端口发射器的优化设计,以实现完全NTM抑制所需的最低功率,与下转向镜的当前设计值相比,下转向镜的环形喷射角要增加几度,而上转向镜的当前设计值要提高几倍。接近最佳。

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  • 来源
    《Nuclear fusion》 |2011年第10期|p.103007.1-103007.15|共15页
  • 作者单位

    FOM Institute for Plasma Physics 'Rijnhuizen', Association EURATOM-FOM, Trilateral Euregio Cluster, PO Box 1207, 3430 BE Nieuwegein, The Netherlands;

    FOM Institute for Plasma Physics 'Rijnhuizen', Association EURATOM-FOM, Trilateral Euregio Cluster, PO Box 1207, 3430 BE Nieuwegein, The Netherlands;

    FOM Institute for Plasma Physics 'Rijnhuizen', Association EURATOM-FOM, Trilateral Euregio Cluster, PO Box 1207, 3430 BE Nieuwegein, The Netherlands;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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