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.
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机译:用等离子体约束实现重力场的动态控制热核聚变(TLTS)方法,通过热辐射等离子体绝缘的壁反应堆防止中子辐射并节省磁场和等离子体的混合,使用旋转磁场的异步磁惯性约束反应堆(AMITYAR和HFM)为实施该方法,在该反应器中点燃热核反应的方法,爆炸式等离子发生器(VIP)的实施方法,以及具有HFM的特立普安瓿,以实现D + T反应和具有超高温热度的HFM D +3НЕ和1Н+11В的高温反应