球点中的弛豫电场

R. M. Mayo, F. Wysocki, J. Fernández
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引用次数: 0

摘要

作者应用边缘螺旋耗散模型的结果(见T.R. Jarboe和B. Alper, 1987)来确定球点弛缓期间电场的相对大小。这是通过量化由通量衰减和弛豫机制产生的等离子体边缘区域的平均电场来实现的。结果表明,边缘处的弛豫电场可达通量衰减场的三倍。该模型还正确地预测,当球标是一个冷的、纯电阻性衰变的物体时,没有弛豫电场。此外,该模型还提供了由弛豫引起的磁衰减功率的估计值,该估计值可高达总衰减功率的75%。
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Relaxation electric fields in spheromaks
The authors apply the results of the edge helicity dissipation model (see T.R. Jarboe and B. Alper, 1987) to determine the relative magnitudes of electric fields during relaxation in spheromaks. This is achieved by quantifying the average electric field in the plasma edge region generated by flux decay and relaxation mechanism(s). It is shown that relaxation electric fields can be as much as three times the flux decay field in the edge. The model also correctly predicts no relaxation electric field when the spheromak is a cold, purely resistively decaying object. In addition, the model provides an estimate for the quantity of magnetic decay power from relaxation, which can be as much as 75% of the total decay power.<>
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