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首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >Experimental and numerical study of the propagation of a discharge in a capillary tube in air at atmospheric pressure
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Experimental and numerical study of the propagation of a discharge in a capillary tube in air at atmospheric pressure

机译:大气压下毛细管中放电在空气中传播的实验和数值研究

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This paper presents an experimental and numerical study of a pulsed air plasma discharge at atmospheric pressure propagating in a capillary glass tube. In this work, we have compared the discharge structures and the axial propagation velocities of discharges. First, we have studied a needle-to-plane configuration without tube. For applied voltages in the range 7-18 kV, we have observed in experiments and in simulations that a plasma ball starts to develop around the needle tip. Then, for applied voltages less than 14 kV, in experiments, the discharge rapidly splits into several streamer channels with a main axial streamer. In simulations, we have computed only the main axial discharge. For applied voltages higher than 14 kV, in experiments and in simulations, we have observed that the discharge propagates with a cone shape in the gap. For all studied voltages, a good experiment/modelling agreement is obtained on the axial propagation velocity of the discharge, which increases with the applied voltage. Then, we have studied the propagation of discharges inside capillary tubes with radii in the range 37.5-300 νm. In experiments and simulations, we have observed that for small tube radius, the discharge front is quite homogeneous inside the tube and becomes tubular when the tube radius increases. Experimentally, we have observed that the velocity of the discharge reaches a maximum for a tube radius slightly less than 100 νm. We have noted that for a tube radius of 100 νm, the discharge velocity is three to four times higher than the velocity obtained without tube. This clearly shows the influence of the confinement by a capillary tube on the discharge dynamics. In this work, we have only simulated discharges for tube radii in the range 100-300 νm. We have noted that both in experiments and in simulations, the velocity of the discharge in tubes increases linearly with the applied voltage. As the radius of the tube decreases, the discharge velocity derived from the simulations slightly increases but is less than the experimental one. We have noted that the discrepancy on the discharge velocity between experiments and simulations increases as the voltage increases.
机译:本文介绍了在大气压下在毛细管玻璃管中传播的脉冲空气等离子体放电的实验和数值研究。在这项工作中,我们比较了放电结构和放电的轴向传播速度。首先,我们研究了没有管的针到平面的配置。对于在7-18 kV范围内施加的电压,我们在实验和模拟中观察到等离子球开始在针尖周围形成。然后,在施加的电压小于14 kV的情况下,在实验中,放电会迅速分离为带有主轴向拖缆的多个拖缆通道。在模拟中,我们仅计算了主轴向流量。对于高于14 kV的施加电压,在实验和模拟中,我们已经观察到放电在间隙中以锥形传播。对于所有研究的电压,在放电的轴向传播速度上都获得了良好的实验/建模协议,该速度随施加的电压而增加。然后,我们研究了毛细管在半径为37.5-300νm的毛细管内部的传播。在实验和模拟中,我们已经观察到,对于较小的管半径,放电前沿在管内部相当均匀,并且在管半径增大时变为管状。从实验上,我们已经观察到,对于略小于100νm的管半径,放电速度达到最大值。我们已经注意到,对于100νm的管半径,放电速度是没有管时获得的速度的三到四倍。这清楚地显示了毛细管限制对放电动力学的影响。在这项工作中,我们仅模拟了100-300νm范围内的管半径放电。我们已经注意到,无论是在实验还是在模拟中,管中的放电速度都随施加的电压线性增加。随着管子半径的减小,从模拟得出的放电速度略有增加,但小于实验值。我们已经注意到,实验和模拟之间的放电速度差异随着电压的增加而增加。

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