Plasma Diamagnetic Effect in Multipole Galatea Trap
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Plasma Diamagnetic Effect in Multipole Galatea Trap
Vol. 42, Issue 12, Pages: 3734-3740(2016)
作者机构:
哈尔滨工业大学电气工程及自动化学院
作者简介:
基金信息:
DOI:
CLC:
Published Online:31 December 2016,
Published:2016
稿件说明:
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TONG Weiming, TAO Baoquan, JIN Xianji, et al. Plasma Diamagnetic Effect in Multipole Galatea Trap[J]. 2016, 42(12): 3734-3740.
DOI:
TONG Weiming, TAO Baoquan, JIN Xianji, et al. Plasma Diamagnetic Effect in Multipole Galatea Trap[J]. 2016, 42(12): 3734-3740.DOI:
Plasma Diamagnetic Effect in Multipole Galatea Trap
摘要
为了在多极Galatea磁阱等离子体约束实验中获得更精确的等离子体参数
利用Rogowski线圈测量了多极磁阱中等离子体的逆磁电流
并借助COMSOL有限元软件分析了磁阱的磁场和等离子体逆磁电流的分布特点
建立了逆磁电流和等离子体分界面处压强之间的数学模型;结合理想气体方程
给出了利用逆磁电流估算等离子体能量约束时间和等离子体温度的方法
并根据测量的逆磁电流计算了不同障壁磁场下多极磁阱中等离子体的主要参数。计算结果表明
障壁磁场磁感应强度在0.025
0
.1 T之间变化时
逆磁电流最大值的变化范围为60
1
10 A
磁阱分界面处压强变化范围为9
1
4 Pa
等离子体的能量约束时间变化范围为50
1
50μs。根据上述测量结果和所提模型估算的等离子体温度约为10 e V
这与热量计测量的等离子体温度基本一致
证明了在等离子体浓度的数值已知的情况下
可以通过测量逆磁电流来测定磁阱中的等离子压强、等离子约束能量时间和等离子体温度。
Abstract
Precise determination of plasma parameters is essential for multipole Galatea magnetic trap experiments. We put forward an experimental method especially based on the diamagnetic diagnosis.The simulation model of multipole Galatea magnetic trap was established and the characteristics of diamagnetic current and pressure distribution in the magnetic trap were analyzed
then a mathematical model was presented combining with the diamagnetic current and plasma separating surface pressure. According to the ideal gas equation
a method of estimating energy confinement time and plasma temperature by using plasma diamagnetic current was also presented. According to the diamagnetic current measured by Rogowski coil and digital integrator and the proposed mathematical model
the dependences of the pressure on the plasma boundary surface
energy confinement time
and plasma temperature for different magnetic field barrier were obtained.The experimental results show that when the barrier magnetic field changes from 0.025 T to 0.1 T
plasma diamagnetic current will change from 60 A to 110 A
the plasma boundary pressure will change from 9 Pa to 14 Pa
plasma energy confinement time will change from 55 μs to 150 μs
and the temperature of the plasma is about 10 e V
which is basically identical with the measured results determined with the help of calorimeter. Calculation results show that under the condition that the plasma concentration values are known
energy confinement time and plasma temperature can be measured by diamagnetic current.