Kremer J P, Pedersen T Sunn, Marksteiner Q, Lefrancois R G, Hahn M
Applied Physics and Applied Mathematics Department, Columbia University, New York, New York 10027, USA.
Rev Sci Instrum. 2007 Jan;78(1):013503. doi: 10.1063/1.2431084.
Techniques for measuring local plasma potential, density, and temperature of pure-electron plasmas using emissive and Langmuir probes are described. The plasma potential is measured as the least negative potential at which a hot tungsten filament emits electrons. Temperature is measured, as is commonly done in quasineutral plasmas, through the interpretation of a Langmuir probe current-voltage characteristic. Due to the lack of ion-saturation current, the density must also be measured through the interpretation of this characteristic thereby greatly complicating the measurement. Measurements are further complicated by low densities, low cross field transport rates, and large flows typical of pure-electron plasmas. This article describes the use of these techniques on pure-electron plasmas in the Columbia Non-neutral Torus (CNT) stellarator. Measured values for present baseline experimental parameters in CNT are phi(p)=-200+/-2 V, T(e)=4+/-1 eV, and n(e) on the order of 10(12) m(-3) in the interior.
描述了使用发射探针和朗缪尔探针测量纯电子等离子体的局部等离子体电势、密度和温度的技术。等离子体电势被测量为热钨丝发射电子时的最小负电势。如同在准中性等离子体中通常所做的那样,通过对朗缪尔探针电流 - 电压特性的解释来测量温度。由于缺乏离子饱和电流,密度也必须通过对该特性的解释来测量,从而使测量大大复杂化。低密度、低横向场输运速率以及纯电子等离子体典型的大流量进一步使测量变得复杂。本文描述了这些技术在哥伦比亚非中性托卡马克(CNT)仿星器中的纯电子等离子体上的应用。CNT 中当前基线实验参数的测量值为:内部的 φ(p)= -200±2 V,T(e)=4±1 eV,以及 n(e)约为 10(12) m(-3) 。