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Pressure profiles of plasmas confined in the field of a magnetic dipole

机译:限制在磁偶极子场中的等离子体压力分布

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Equilibrium pressure profiles of plasmas confined in the field of a dipole magnet are reconstructed using magnetic and x-ray measurements on the levitated dipole experiment (LDX). LDX operates in two distinct modes: with the dipole mechanically supported and with the dipole magnetically levitated. When the dipole is mechanically supported, thermal particles are lost along the field to the supports, and the plasma pressure is highly peaked and consists of energetic, mirror-trapped electrons that are created by electron cyclotron resonance heating. By contrast, when the dipole is magnetically levitated losses to the supports are eliminated and particles are lost via slower cross-field transport that results in broader, but still peaked, plasma pressure profiles.
机译:使用磁悬浮和偶极子实验(LDX)上的磁性和X射线测量来重建局限在偶极子磁体场中的等离子体的平衡压力曲线。 LDX以两种不同的模式工作:机械支撑偶极子和磁悬浮磁偶极子。当偶极子受到机械支撑时,热粒子会沿着磁场损失到支撑物上,等离子压力会达到最高峰,并由电子回旋共振加热产生的高能镜陷电子组成。相反,当偶极子磁悬浮时,消除了对载体的损失,并且通过较慢的交叉场传输而损失了颗粒,从而产生了较宽但仍处于峰值的等离子体压力曲线。

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