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Experimental Investigation of High Temperature High Voltage Thermionic Diode for the Space Power Nuclear Reactor

机译:空间电力核反应堆高温高压热太极二极管的实验研究

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It is well known that the rise of arc from the dense glow discharge is connected with the thermion and secondary processes on the cathode surface (Granovsky, 1971; Leob, 1953; Engel, 1935). First model of breakdown of the cathode layer is connected with the increase of the cathode temperature in consequence of the ion bombardment that leads to the grows its thermo-emissive current. Other model shows the main role of the secondary effects on the cathode surface - the increase of the secondary ion emission coefficient - γ_i with the grows of glow discharge voltage. But the author of this investigation work of breakdown in Cs vapor (a transmission the glow discharge into self-maintaining arc discharge) discovered the next peculiarity: the value of breakdown voltage is constant when the values of vapor temperature (its pressure p_(cs)) and cathode temperature T_k is constant too (U_b = constant with T_k = constant and p_(cs) = constant) and it is not a statistical value (Onufryev, Grishin, 1996) (that was observed in gas glow discharges other authors (Granovsky, 1971; Leob, 1953; Engel, 1935)). The investigations of thermion high voltage high temperature diode (its breakdown characteristics in closed state and voltage-current characteristics in disclosed state) showed that the value of the breakdown voltage is depended on the vapor pressure in inter-electrode gap (IEG) - p_(cs) and cathode temperature -T_k and is independent on IEG length - Δ_(ieg). On this base it was settled that the main role in transition of glow discharge to self-maintaining arc discharge plays an ion cathode layer but more exactly - the region of excited atoms -"Aston glow".
机译:众所周知,来自致密辉光放电的弧的升高与阴极表面上的热电源和次要过程(Granovsky,1971; Leob,1953; Engel,1935)连接。由于离子轰击导致其热发射电流的离子轰击,阴极层的第一模型与阴极温度的增加相连。其他模型显示了二次效果对阴极表面的主要作用 - 二次离子发射系数 - γ_I的增加随着辉光放电电压的增长。但是,在CS蒸汽崩溃的作者中,CS蒸汽崩溃的作品(传播到自我保持电弧放电中的发光放电)发现了下一个特殊性:当蒸汽温度的值(其压力P_(CS)时,击穿电压的值是恒定的)和阴极温度T_K也是恒定的(U_B =与T_K =常数的常数和P_(CS)=常数),并且它不是统计值(ONUFRYEV,GRISHIN,1996)(在气体发出中观察到其他作者(Granovsky) ,1971年; Leob,1953; Engel,1935))。热电激的高压高温二极管的研究(其闭合状态下的击穿特性以及所公开状态的电压 - 电流特性)显示击穿电压的值依赖于电极间隙中的蒸气压(IEG) - P_( CS)和阴极温度-T_K并独立于IEG长度 - Δ_(IEG)。在该基础上,它稳定在发光放电转变为自维持电弧放电的主要作用起到了离子阴极层,但更准确地 - 激发原子区域 - “阿斯顿辉光”。

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