RAN Junxia, MA Dong, LUO Haiyun, et al. Evolution of Air Uniform Dielectric Barrier Discharge at Atmospheric Pressure and Its α Coefficient Measurement[J]. 2018, 44(3): 876-880.
RAN Junxia, MA Dong, LUO Haiyun, et al. Evolution of Air Uniform Dielectric Barrier Discharge at Atmospheric Pressure and Its α Coefficient Measurement[J]. 2018, 44(3): 876-880.DOI:
大气压空气均匀介质阻挡放电的演化及α系数测量
摘要
为实现较大间隙下的大气压空气介质阻挡均匀放电
通过ICCD高速相机研究了大气压空气均匀放电随时间的演化过程
并利用光学方法测量了大气压空气的电子碰撞电离系数(α系数)。ICCD高速时间分辨图像表明
大气压空气中的均匀放电是由汤森放电起始
随着放电的发展逐渐增强
当电流达到峰值时刻
放电也最强
但仍然为汤森放电。利用汤森放电阶段拍摄的纳秒级曝光时间的序列发光图像
对α系数进行了测量
测量了E/p0为29
3
2 V/(m·Pa)范围的大气压空气中的α系数。测量结果表明
α/p0与E/p0在一定范围内有函数关系
不同研究者在相同约化电场下测量得到的α/p0数值是接近的
至于细微的差别
一是来源于各自测量方法的不同
二是由于空气的附着系数在低E/p0值下十分分散
这也导致α系数的有效值也比较分散。该结果补充了低E/p0下α系数实验数据的空白。
Abstract
In order to achieve uniform dielectric barrier discharge at atmospheric pressure under large air gap
the evolution of air uniform discharge at atmospheric pressure was studied by means of ICCD high speed camera. The α coefficient of atmospheric air was measured by optical method. It is shown that the uniform discharge in atmospheric air is Townsend discharge throughout the discharge process. The discharge increases with the development of the applied voltage. The discharge intensity reaches the strongest when the current reaches the peak time.Moreover
the distribution of the light intensity in the discharge gap was recorded by taking side-view photograph using an ICCD camera with an extremely short exposure time and compared with the theoretical distributions
with different presumed α. The value of α was determined by the best fitting of the theoretical distribution to the experimental one
and was measured in atmospheric pressure air in the range of 29
3
2 V/(m·Pa) by using the light emission images. The results show that α/p0 and E/p0 in a certain range has a function relationship. The results of different studies in the same reduced field E/p0 are similar.The subtle differences come from two aspects:(1) their methods of measurement are different
(2)the air electronic attachment coefficient at low E/p0 value is very dispersed
thus the alpha coefficients of valid values are more scattered.