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The oak ridge thermonuclear program-recent advances on the DCX

机译:橡树岭热核计划-DCX的最新进展

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摘要

In the Oak Ridge thermonuclear experiment, 600. kev molecular ions of hydrogen or deuterium are injected into the median plane of a direct current magnetic mirror machine (DCX). A fraction of the molecular ions is dissociated (H2+ ș2; H+ + Ho) as the ion beam passes through a high-energy carbon arc whose electrodes are located at each end of DCX. The magnetic field configuration is such that the 300-kev atomic ions thus created are trapped by virtue of the change in charge-to-moss ratio and enter a circular orbit concentric with the magnetic axis. The neutral atoms and the remaining undissociated molecular beam leave the machine. Loss processes, principally charge exchange collisions suffered by the circulating ions, have thus far prevented achieving the appreciable plasma density required for observable fusion reactions. Plasma densities In the order of 10+10 ions/cm3 and mean containment times of 10 to 12 msec have been observed. The experimental program at the present time is one of diagnostic measurements on the trapped ions and their environment, and of building up the plasma density by increasing the trapping rate and containment time.
机译:在Oak Ridge热核实验中,将600. kev的氢或氘分子离子注入直流磁镜机(DCX)的中位平面。当离子束穿过电极位于DCX两端的高能碳弧时,一部分分子离子被分解(H2 ++ 2; H + + Ho)。磁场结构使得这样产生的300kev原子离子由于电荷与苔藓比的变化而被俘获,并进入与磁轴同心的圆形轨道。中性原子和其余未解离的分子束离开机器。迄今为止,损失过程,主要是循环离子所遭受的电荷交换碰撞,一直无法实现可观察到的聚变反应所需的可观的等离子体密度。等离子体密度约为10 + 10离子/ cm3,平均容纳时间为10到12毫秒。目前的实验程序是对捕获离子及其周围环境的诊断测量之一,以及通过增加捕获速率和抑制时间来建立等离子体密度的方法之一。

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