EFFECT OF AIR ADMIXTURE IN HELIUM ON THE RATE OF THE BREAKDOWN CURRENT RISE

被引:14
作者
BARTNIKAS, R
NOVAK, JP
机构
[1] UNIV WATERLOO,WATERLOO N2L 3G1,ONTARIO,CANADA
[2] ECOLE POLYTECH,MONTREAL H3C 3A7,QUEBEC,CANADA
[3] MCGILL UNIV,MONTREAL H3A 2T5,QUEBEC,CANADA
关键词
D O I
10.1109/27.163585
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The influence of dry air admixtures upon the breakdown mechanism of helium in small gap separations was investigated, using plane parallel stainless-steel electrodes enclosed within a Pyrex chamber. The test chamber was evacuated to a limit pressure of 10(-5) torr and the electrodes degassed under a glow discharge. All experiments were carried out under atmospheric pressure, with the additions of air being made at relative partial pressures of p(r) = 0, 10(-4), 3 x 10(-4), 10(-3), and 3 x 10(-3). The initial breakdown current was measured by means of a digital oscilloscope and the semilogarithmic plots of the discharge current as a function of time (up to ca. 100muA) were found to exhibit an exponential dependence. The reciprocal value of the time constant of the breakdown current rise, tau-1, was demonstrated to vary in accordance with the linear relation tau-1 = tau(o)-1 p(r)m DELTAV for an overvoltage DELTAV = V - V(b) (for V > V(b), V(b) being the breakdown voltage) in the range between zero to ca. 35 V; a log-log plot of tau-1 versus the applied voltage, DELTAV, with relative partial pressure p(r) as a parameter was shown to lead the empirical relationship tau0(-1) = 3.11p(r)0.6 (s-1 V-1) valid within the range from ca. 10(-4) to 3 x 10(-3). The values of the breakdown voltage were determined from the extrapolated intercepts of the tau-1 versus the applied voltage, V, characteristics. The experimental rate of rise of the breakdown current was compared with the theoretical current growth, calculated using a two-dimensional model of the breakdown process. The calculations were performed at p(r) = 10(-4) with DELTAV = 33 V. It has been found that the rate of rise of the calculated current exceeds the experimental one by a factor of about 2.6, but agrees quite satisfactorily with the value that is obtained when the experiment is conducted at p(r) = 3 x 10(-4).
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页码:487 / 492
页数:6
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