水中针-板结构小能量脉冲火花放电特性

王芝; 韩若愚; 李显东; 陈鹏宇; 李奕璋; 缪劲松

doi:10.11884/HPLPB202234.220022

水中针-板结构小能量脉冲火花放电特性

doi: 10.11884/HPLPB202234.220022

1.
北京理工大学物理学院，北京 100081
2.
重庆大学电气工程学院，重庆 400044

基金项目: 北京市自然科学基金项目(3212034)；国家自然科学基金项目(51907007)

详细信息

作者简介:
王　芝，380810708@qq.com

通讯作者:
韩若愚，han.ruoyu@hotmail.com

中图分类号: TM89
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- 被引次数: 0
出版历程
- 收稿日期: 2022-01-11
- 修回日期: 2022-04-24
- 网络出版日期: 2022-04-30
- 刊出日期: 2022-06-17

Low-energy pulsed spark discharge characteristics of pin-plate structure in water

1.
School of Physics, Beijing University of Technology, Beijing 100081 , China
2.
School of Electrical Engineering, Chongqing University, Chongqing 400044, China

摘要

摘要: 开展了J量级系统储能下电脉冲参数对水中火花放电特性影响研究。驱动源采用参数可调的固态重频纳秒脉冲电源，放电负载为水中针-板结构（间距1 mm），在低重频条件（约5 Hz）下进行实验。通过调节放电参数、拍摄高速阴影图像、光谱诊断以及声信号测量，研究水中脉冲放电的物理特性，得到不同放电参数下放电演化规律及其对声学、光谱特性影响。实验发现：在J量级储能下，放电通道连通两极后，回路电流在几百ns内快速上升至10 A左右，随后缓慢下降，持续50～60 μs。发现预设脉宽对放电影响较大，短脉宽条件下放电会被电源固态开关强制截断出现反向放电，而长脉宽条件下放电通道在后期变得不稳定甚至熄弧中断，出现气泡中二次放电现象。辐射光谱揭示了更多等离子体信息，推断通道电子密度在10¹⁸ cm⁻³量级，随着脉宽增加，特征谱线强度增加，表明活性粒子数密度增加，但粒子种类不变。短脉冲（＜150 μs）作用下产生的脉冲声波的特征宽度在110～150 μs，而当脉宽继续增大，声波脉宽并不继续增加而是保持不变，保持在150 μs左右。研究结果对水中小能量火花放电的机理研究有一定参考价值，为水声学、液相等离子体等领域的应用提供思路。
- 水中放电 /
- 等离子体 /
- 图像诊断 /
- 光谱诊断 /
- 声波与冲击波
Abstract: The influence of electric pulse parameters on spark discharge characteristics in water was studied. A solid-state repetitive nanosecond pulse power supply with adjustable parameters was adopted. The discharge load was a pin-plate structure placed in water (the distance between the pin and the plate set to 1 mm). The experiment was carried out under low repetitive frequency conditions (approximately 5 Hz). The characteristics of pulse discharge in water were obtained by monitoring discharge parameters, taking high-speed shadow images, collecting optical emission spectrum, and measuring sound pressure. The evolution of pulse discharge with different parameters and its influence on acoustic and spectral characteristics were also obtained. When the energy storage on the order of a few joules after the initial discharge channel was formed between the two electrodes, the circuit current rose to approximately 10 A within a few hundred ns, followed by a rapid and then slow decline with a duration of 50−60 μs. It is found that the preset pulse width has a great influence on the spark discharge characteristics. Under short pulse width conditions, the discharge channel will be cut off by the solid-state switch of the power supply. Under long pulse width conditions, the discharge channel becomes unstable in the late stage and even interrupts the arc,and the secondary discharge appears in bubbles. The radiation spectra reveal more information. With the increase of pulse width, the intensity of the characteristic spectral lines increased, but no new spectral lines were observed. This indicates that the number of active particles increased, and their types remain the same.The channel electron density is estimated on the order of 10¹⁸ cm⁻³. The characteristic width of the pulse sound wave produced by a short pulse (＜150 μs) is 110−150 μs. However, when the pulse width continues to increase, the sound wave pulse width does not continue to increase but remains at 150 μs. It is hoped that this research has a certain reference value for studying the mechanism of small energy spark discharge, and provides ideas for the applications of underwater acoustics, liquid phase plasma and other fields.
- discharge in water /
- plasma /
- image diagnosis /
- spectral diagnosis /
- sound and shock waves

HTML全文

图 1 实验装置图

Figure 1. Schematic diagram of experimental device

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图 2 针-板火花放电波形图

Figure 2. Pin-plate spark discharge waveform diagram

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图 3 针-板火花放电过程

Figure 3. Pin-plate spark discharge process

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图 4 针-板火花放电光谱图

Figure 4. Pin-plate spark discharge spectra

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图 5 针-板火花放电声学图

Figure 5. Acoustic diagram of the pin-plate spark discharge

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