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Flow Dynamics and Plasma Heating of Spheromaks in SSX

机译:SSX中球状球的流动动力学和等离子体加热

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We report several new experimental results related to flow dynamics and heating from single dipole-trapped spheromaks and spheromak merging studies at SSX. Single spheromaks (stabilized with a pair of external coils, see Brown, Phys. Plasmas 13 102503 (2006)) and merged FRC-like configurations (see Brown, Phys. Plasmas 13, 056503 (2006)) are trapped in our prolate (R = 0.2 m, L = 0.6 m) copper flux conserver. Local spheromak flow is studied with two Mach probes (r_1 ≤ ρ_i r_2 ≥ ρ_i calibrated by time-of-flight with a fast set of magnetic probes at the edge of the device. Both Mach probes feature six ion collectors housed in a boron nitride sheath. The larger Mach probe will ultimately be used in the MST reversed field pinch. Line averaged flow is measured by ion Doppler spectroscopy (IDS) at the midplane. The SSX IDS instrument measures with 1 μs or better time resolution the width and Doppler shift of the C_(III) impurity (H plasma) 229.7 nm line to determine the temperature and line-averaged flow velocity (see Cothran, RSI 77, 063504 (2006)). We find axial flows up to 100 km/s during formation of the dipole trapped spheromak. Flow returns at the wall to form a large vortex. Recent high-resolution IDS velocity measurements during spheromak merging show bi-directional outflow jets at ±40 km/s (nearly the Alfven speed). We also measure T_i ≥ 80 eV and T_e ≥ 20 eV during spheromak merging events after all plasma facing surfaces are cleaned with helium glow discharge conditioning. Transient electron heating is inferred from bursts on a four-channel soft x-ray array. The spheromaks are also characterized by a suite of magnetic probe arrays for magnetic structure B(r,t), and interferometry for n_e. Finally, we are designing a new oblate, trapezoidal flux conserver for FRC studies. Equilibrium and dynamical simulations suggest that a tilt-stable, oblate FRC can be formed by spheromak merging in the new flux conserver.
机译:我们报告了一些新的实验结果,这些结果来自于单个偶极子捕获的球状体和SSX中的球状体合并研究中的流动动力学和加热。单个球状体(用一对外部线圈稳定,请参见Brown,物理等离子13 102503(2006))和合并的FRC样配置(请参见Brown,Phys。Plasmas 13,056503(2006))被困在我们的扁长(R = 0.2 m,L = 0.6 m)。用两个Mach探针(飞行时间校准过的r_1≤ρ_ir_2≥ρ_i)和设备边缘的一组快速磁性探针研究了局部的球面渗流,这两个Mach探针都具有六个离子收集器,这些离子收集器位于氮化硼鞘中。较大的Mach探头最终将用于MST反向场收缩中。通过离子多普勒光谱仪(IDS)在中平面测量线平均流量; SSX IDS仪器以1μs或更佳的时间分辨率测量宽度和多普勒频移。用C_(III)杂质(H等离子体)229.7 nm线确定温度和线平均流速(请参阅Cothran,RSI 77,063504(2006))。偶极子俘获的球状球体,流动返回壁形成一个大漩涡,球状球体合并期间最近的高分辨率IDS速度测量显示双向流出射流的速度为±40 km / s(接近Alfven速度),我们也测量到T_i≥80球囊合并术中eV和T_e≥20 eV使用氦气辉光放电清洁剂清洁所有面对等离子体的表面后,再进行操作。从四通道软X射线阵列上的爆发可以推断出瞬态电子加热。椭球体的特征还在于用于磁性结构B(r,t)的一组磁性探针阵列和用于n_e的干涉测量法。最后,我们正在为FRC研究设计一个新的扁圆形梯形通量储能器。平衡和动力学模拟表明,可以通过在新的通量容器中合并球状球形成倾斜稳定的扁圆FRC。

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