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首页> 外文期刊>Physics of plasmas >The effects of plasma density and magnetic field on ion temperature and drift velocity in a LaB6 direct current plasma
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The effects of plasma density and magnetic field on ion temperature and drift velocity in a LaB6 direct current plasma

机译:等离子体密度和磁场对LaB6直流等离子体中离子温度和漂移速度的影响

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摘要

In a LaB6 direct current plasma, parallel and perpendicular ion temperatures (T-i parallel to and T-i perpendicular to) were measured as a function of plasma density and magnetic field by a laser-induced fluorescence technique. In order to study the impacts of magnetic field and plasma density on ion temperature and drift velocity, the plasma density was controlled by a magnetic field and discharge current under the following plasma conditions: The magnetic field intensity at the measurement position, B-D, was 186-405 G; discharge voltage, V-dis, was 29.9-32.1 V; discharge current, I-dis, was 10-22 A; neutral pressures, P-n, were 130 mTorr (in the source region) and 2.2 mTorr (at diagnostic region); plasma density, n(p), was (2-8)x10(12) cm(-3); and electron temperature, T-e, was similar to 2.6 eV. Parallel ion temperature (T-i parallel to), perpendicular ion temperature (T-i perpendicular to), and drift velocity, v(D parallel to) (or drift kinetic energy, E-D) all increase as a function of B-D and I-dis, such that the total ion energy, E-t (=T-i perpendicular to+T-i parallel to+E-D), increases as a function of B-D and I-dis. From the relations of T-i parallel to, T-i perpendicular to, and v(D parallel to) to n(p), ion temperature and drift velocity were observed to be strongly depend on plasma density. In consideration of the collision time scales, ion gyrofrequency, and time of flight from the source to the measurement position, the dominant process for ion heating was observed to be the electron-ion collisions, although the magnetic field and ion-neutral collisions contribute to ion temperature anisotropy.
机译:在LaB6直流等离子体中,通过激光诱导荧光技术测量平行和垂直离子温度(平行于T-i和垂直于T-i)作为等离子体密度和磁场的函数。为了研究磁场和等离子体密度对离子温度和漂移速度的影响,在以下等离子体条件下,通过磁场和放电电流控制等离子体密度:测量位置BD的磁场强度为186 -405 G;放电电压V-dis为29.9-32.1 V;放电电流I-dis为10-22 A;中性压力P-n为130 mTorr(在源区)和2.2 mTorr(在诊断区);血浆密度n(p)为(2-8)x10(12)cm(-3);电子温度T-e约为2.6 eV。平行离子温度(Ti平行),垂直离子温度(Ti垂直)和漂移速度v(D平行)(或漂移动能ED)都随BD和I-dis的增加而增加,因此总离子能Et(=垂直于Ti的Ti +平行于+ ED的Ti)随BD和I-dis的增加而增加。从平行于T-i,垂直于T-i和与n(p)的v(D)的关系,可以观察到离子温度和漂移速度很大程度上取决于等离子体密度。考虑到碰撞的时间尺度,离子的陀螺频率和从离子源到测量位置的飞行时间,尽管磁场和离子中性的碰撞对电子的碰撞产生了影响,但离子加热的主要过程还是电子-离子碰撞。离子温度各向异性。

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