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The forming of intensive metal ion flows in plasma beam discharge

机译:等离子束放电中强金属离子流的形成

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Summary form only given. The process of dense metal ion flows withenergy in the range 102-103 eV in a plasma beamdischarge in the plasma break-down of disruptive distance is studied.The creation of metal vapor was possible at the expense of heating ofthe metal test piece, inserted into a primary gas discharge plasma bymeans of supplying of voltage up to 103 V as to plasmapotential and forming the ion flows on the test piece. After attainmentof boiling temperature we can see the sudden increase at metal atomsnear the test piece and the creation of a dense metal plasma due tovapor ionization by accelerated electrons. With the occurence of a densesurface secondary plasma `pushing away' the electric field from theevaporating test piece, a double electric layer of space charge occurson the interface between these two plasmas. It forms the primary plasmaelectron flows and secondary plasma ion flows. The energy of the chargedparticles is regulated by changing the voltage on the evaporatingtest-piece. The metal ion current value and electron current value areregulated by changing the concentration of primary gas discharged plasma
机译:仅提供摘要表格。致密金属离子流过的过程 等离子束中的能量在10 2 -10 3 eV范围内 研究了等离子体破坏中的放电破坏距离。 金属蒸气的产生是可能的,但要以加热金属为代价。 金属试件,通过以下方式插入一次气体放电等离子体中: 向等离子提供高达10 3 V的电压的方式 电位并在试件上形成离子流。达到之后 沸腾温度的变化,我们可以看到金属原子突然增加 靠近测试件并由于以下原因产生了致密的金属等离子体 通过加速电子进行蒸汽电离。随着密集的发生 表面次级等离子体从电极上推电场。 蒸发试件时,会发生空间电荷的双电层 在这两个等离子体之间的界面上。它形成主要血浆 电子流和二次等离子体离子流。带电的能量 通过改变蒸发上的电压来调节颗粒 试件。金属离子电流值和电子电流值分别为 通过改变一次气体放电等离子体的浓度进行调节

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