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Validation of the current decay model in the initial phase of current quench in high β_p disruptive discharges of JT-60U

机译:JT-60U高β_P中断排放中电流淬火初始阶段电流衰减模型的验证

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The precise prediction of plasma current decay time, T, is important in order to estimate the electromagnetic forces acting on vacuum vessel and in-vessel components during the tokamak disruption. The so-called LIR model often used to predict the current decay time in ITER [1] is based on a simple series circuit considering the plasma resistance R_p and inductance L_p, which are constant in time. In the "LIR model", the current decay time represents with τ_(L/r) = L_p/R_p. If the plasma resistivity is defined by Spitzer resistivity [2], the current decay time is mainly determined by the electron temperature T_e and effective charge Z_(eff). However, the systematic research of the relationship between the current decay time during disruption and the measurement value of L_p and R_p has rarely been done until now.
机译:等离子体电流衰减时间T的精确预测是重要的,以估计在Tokamak中断期间在真空容器和容器组分上作用的电磁力。考虑到等离子体电阻R_P和电感L_P的简单串联电路,经常用于预测迭代中的所谓的LIR模型是基于简单的串联电路。在“LIR模型”中,当前衰减时间与τ_(l / r)= l_p / r_p表示。如果溅射电阻率限定等离子体电阻率[2],则电流衰减时间主要由电子温度T_E和有效电荷Z_(EFF)确定。然而,目前衰变时间与L_P和R_P的测量值之间的关系的系统研究很少完成。

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