首页> 外文期刊>Journal of Plasma Physics >Spectral dependence, efficiency and localization of non-inductive current drive via helicity injection by global Alfvén waves in tokamak plasmas
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Spectral dependence, efficiency and localization of non-inductive current drive via helicity injection by global Alfvén waves in tokamak plasmas

机译:托卡马克等离子体中的全局Alfvén波通过螺旋注入注入的非感应电流驱动的光谱依赖性,效率和局部性

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摘要

A systematic study of non-inductive current drive via helicity injection by global Alfvén eigenmode (GAE) waves is carried out. For illustration, the first radial mode of the discrete resonant GAE spectrum is considered. The following aspects are given special attention: spectral analysis, radial dependence and efficiency – all of these as functions of the characteristics of the waves launched by an external, concentric antenna (i.e. wave frequency and poloidal and toroidal wavenumbers). The tokamak plasma is simulated by a current-carrying cylindrical plasma column surrounded by a helical sheet current and situated inside a perfectly conducting shell, with incorporation of equilibrium (simulated) toroidal field, magnetic shear and a relatively large poloidal magnetic field component. Within the framework of low-[beta] MHD model equations and for typical tokamak physical parameters, the following basic results are obtained: (1) in the range of poloidal wavenumbers [minus sign]3[less-than-or-eq, slant]m[less-than-or-eq, slant]3 and toroidal wavenumbers [minus sign]20[less-than-or-eq, slant]n[less-than-or-eq, slant]20, resonant GAE peaks below the Alfvén continuum are found; (2) the power absorption (P), current drive (I) and corresponding frequency of the GAE modes depend strongly on the sets of (m, n) values considered; (3) the ‘net’ current drive is positive (i.e. flows in the direction of the equilibrium current j0z) for m=[minus sign]1, [minus sign]2, [minus sign]3 and [minus sign]20[less-than-or-eq, slant]n[less-than-or-eq, slant][minus sign]1 as well as for m=+1, +2, +3 and n>10; (4) in the cases m=[minus sign]1, [minus sign]2, [minus sign]3, the efficiency of current drive, I/P, increases with [mid R:]m[mid R:] and 1/[mid R:]n[mid R:]; (5) the radial localization of the current drive in each of the cases considered is determined and tabulated.
机译:对全球Alfvén本征模(GAE)波通过螺旋注入进行的无感电流驱动进行了系统研究。为了说明,考虑了离散谐振GAE频谱的第一径向模式。需要特别注意以下几个方面:频谱分析,径向相关性和效率–所有这些都与外部同心天线发射的波的特征有关(即波频率以及多极化和环形波数)。托卡马克等离子体是由载流的圆柱形等离子体柱模拟的,该柱等离子体柱被螺旋薄层电流包围,并位于一个完全导电的壳内部,并结合了平衡的(模拟的)环形场,磁剪切力和相对较大的极化磁场分量。在低βMHD模型方程的框架内,对于典型的托卡马克物理参数,可获得以下基本结果:(1)在极谱波数[负号] 3 [小于或等于,斜率]范围内] m [小于或等于,倾斜] 3和环形波数[负号] 20 [小于或等于,倾斜] n [小于或等于,倾斜] 20,共振GAE峰在Alfvén连续体下面; (2)GAE模式的功率吸收(P),电流驱动(I)和相应的频率在很大程度上取决于所考虑的(m,n)个值集; (3)当m = [负号] 1,[负号] 2,[负号] 3和[负号] 20 []时,“净”电流驱动为正(即,朝平衡电流j0z的方向流动)。小于或等于斜率] n [小于或等于斜率] [负号] 1以及m = + 1,+ 2,+ 3和n> 10时; (4)在m = [负号] 1,[负号] 2,[负号] 3的情况下,电流驱动I / P的效率随[mid R:] m [mid R:]和1 / [mid R:] n [mid R:]; (5)确定并列出每种情况下当前驱动器的径向定位。

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