The dynamic evolution of atmospheric-pressure pulsed air discharge over a water droplet
Zhiguo Zhao, Dongping Liu, Yang Xia, Guofeng Li, Chunjie Niu, Zhihua Qi, Xi Wang, Zilu Zhao
Abstract
Zhiguo Zhao, Dongping Liu, Yang Xia, Guofeng Li, Chunjie Niu, Zhihua Qi, Xi Wang, Zilu Zhao
Abstract
In this paper, a pin-to-plate reactor with a water droplet as a suspended electrode is employed to investigate the dynamic evolution of pulsed air discharge over the water droplet. The temporal and spatial evolution of the pulsed discharge is captured by an intensified charge-coupled device (ICCD) camera, and the spatial distribution of the electric field is obtained by solving the Maxwell equations. Our ICCD measurements show that the discharge is initiated in the gas gap between the anode and the droplet, and then it propagates over the droplet. Our simulation confirms that the strong electric field is formed when the water droplet is placed in the gas space. The propagation of air discharge over the water droplet anode-directed and its propagation velocity is on the order of 1.8 × 105 m s−1. With a decrease in the applied voltage, the long duration of air discharge is formed in the gas space, which could be related to the diffusion-controlled combination of charges remaining in the water droplet.
OpenAlex reports 10 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
In this paper, a pin-to-plate reactor with a water droplet as a suspended electrode is employed to investigate the dynamic evolution of pulsed air discharge over the water droplet. The temporal and spatial evolution of the pulsed discharge is captured by an intensified charge-coupled device (ICCD) camera, and the spatial distribution of the electric field is obtained by solving the Maxwell equations. Our ICCD measurements show that the discharge is initiated in the gas gap between the anode and the droplet, and then it propagates over the droplet. Our simulation confirms that the strong electric field is formed when the water droplet is placed in the gas space. The propagation of air discharge over the water droplet anode-directed and its propagation velocity is on the order of 1.8 × 105 m s−1. With a decrease in the applied voltage, the long duration of air discharge is formed in the gas space, which could be related to the diffusion-controlled combination of charges remaining in the water droplet.
Key concepts: Streamer discharge, Anode, Electric field, Electric discharge in gases, Physics, Diffusion, Atmospheric pressure, Mechanics