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Plasma dynamics of an explosive emission center - ecton of a cathode spot in external tangential magnetic field

机译:外部切向磁场中阴极点爆炸发射中心-等离子体的等离子体动力学。

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The plasma dynamics of an explosive-emission center demonstrates the plasma polarization in applied external magnetic field, induced by dense plasma spherical expansion across the magnetic field. The additional positive space charge appears at the retrograde side of the dense plasma due to the polarization current jϕ=σBv/c ≈105BT [A/cm2]. Probability of initiation of a new explosive emission center increases at the retrograde side and decreases at the amperian side due to this polarization. Velocity of a cathode spot retrograde motion (for considered copper cathode) vretr was estimated as vretr∼0.3·vrandom·BT. For a clean surface vrandom ∼104cm/s, hence vretr ∼0.3BGs [cm/s]. The “Robson angle” function was derived from simple geometrical reasons of the spot-cell (explosive-emission-center) plasma polarization, i.e. ζR=arctan(A·tanθB), where A≡tanαpl/cosαpl and αpl = 20°–40° - plasma-jet-expansion parameter. Therefore, considering of a plasma dynamics of the explosive-emission center can give an explanation of the vacuum-arc cathode-spot retrograde motion in frames of the ecton model.
机译:爆炸物发射中心的等离子体动力学表明,施加的外部磁场中的等离子体极化是由磁场中密集的等离子体球形膨胀引起的。由于极化电流j ϕ =σBv/ c≈105BT[A / cm 2 ],额外的正空间电荷出现在致密等离子体的逆行侧。由于这种极化,新的爆炸物发射中心启动的可能性在逆行侧增加,而在安培侧减小。阴极点逆行运动的速度(对于考虑的铜阴极而言)vretr估计为v retr 〜0.3·v 随机·BT。对于干净的表面v 随机 〜10 4 cm / s,因此v retr 〜0.3B Gs [cm / s]。 “罗布森角”函数源自点细胞(爆炸发射中心)等离子体极化的简单几何原因,即ζ R = arctan(A·tanθ B ),其中A≡tanα pl /cosα pl 和α pl = 20°–40°-等离子流膨胀参数。因此,考虑到爆炸物发射中心的等离子体动力学,可以解释在ecton模型框架中真空弧阴极点逆行运动。

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