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交流电的放电特性详细资料说明

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采用蜂窝状排列的七个帽状射流的二维阵列装置,设计了以单电极结构为基本等离子体射流的冷空气等离子体(CAP)射流阵列。这项工作的动机是利用本来就很小的大气等离子体来解决许多大规模处理应用的挑战。基于详细的电学、光谱和成像特性,研究了等离子体射流阵列的放电特性。结果表明,帽状射流阵列具有良好的时间射流均匀性。此外,本文还通过两组增强型电荷耦合器件的图像,对射流放电的动力学行为进行了详细的研究。研究发现,这7种射流具有良好的时间同步性和射流均匀性,同时具有丰富的射流相互作用动力学特性,如射流头附近有轻微的斥力,特别是在氦气流量较小的情况下。这些动态特性为更好地控制射流相互作用和进一步优化大规模帽源设计提供了可能的见解。

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交流电的放电特性详细资料说明.pdf 455K

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1724  
IEEE TRANSACTIONS ON PLASMA SCIENCE, VOL. 40, NO. 6, JUNE 2012  
Discharge Characteristics of a  
Cold-Atmospheric-Plasma Jet Array Generated  
With Single-Electrode Configuration  
Qian-Qian Fan, Mu-Yang Qian, Chun-Sheng Ren, Dezhen Wang, and Xiaoqiong Wen  
Abstract—In this paper, a cold atmospheric plasma (CAP) jet  
array is generated by a 2-D array device of seven CAP jets  
arranged in a honeycomb configuration and designed with single-  
electrode configuration as the elemental plasma jet. The work is  
motivated by the challenge of using inherently small atmospheric  
plasmas to address many large-scale processing applications. The  
discharge characteristics of the plasma jet array are investigated  
based on detailed electrical, spectroscopic, and imaging charac-  
terizations. The CAP jet array is shown to achieve good temporal  
jet–jet uniformity. Furthermore, the dynamic behavior of the jet  
discharges is studied particularly through two series of intensified-  
charge-coupled-device images taken at the end views. It has been  
found that the seven jets show a good temporal synchronization  
and jet–jet uniformity, as well as rich dynamics of jet–jet in-  
teractions such as a slight repulsion at surrounding jet heads,  
particularly for a small gas flow rate of helium. These dynamic  
features offer possible insights with which to better control the  
jet–jet interactions and further optimize the design of large-scale  
CAP sources.  
Index Terms—Plasma, plasma diagnosis, plasma jet array.  
Fig. 1. Schematic of the CAP jet array configuration with both (left) side view  
and (right) end view.  
I. INTRODUCTION  
this kind of application is by grouping many CAP jets together  
to form an array of plasma jets. While extensive studies and  
considerable advance have been made with individual plasma  
jets [8]–[19], CAP jet arrays are far less studied [20]–[25].  
Driven by the exciting prospects for a range of commercial  
large-scale applications, several cold-plasma jet array devices  
of scalable 1-D and 2-D arrays have been designed by Lu et al.  
[22], Cao et al. [23], [24], and Nie et al. [25]. These plasmas  
are capable of a direct production of reactive species near large-  
scale 3-D objects with tight control of plasma stability, which  
are generated with capillary–ring electrode configuration or  
with a downstream ground electrode. Our work aims to develop  
a 2-D CAP jet array with single-electrode configuration as  
the elemental plasma jet and with its ability to treat complex  
3-D heat-sensitive biomedical material. Properties of the jet  
array discharge are investigated by means of detailed electrical,  
spectroscopic, and imaging diagnoses. The rest of this paper is  
organized as follows. The experimental setup is described in  
Section II. Details of the experimental results are presented in  
Section III. Finally, the conclusions are given in Section IV.  
OWADAYS, utilization of cold atmospheric plasmas  
(CAPs) is studied with growing interest, and many con-  
N
figurations and applications are investigated for its remarkable  
advantages compared with plasma applications in vacuum sys-  
tems, such as low operating cost, reduction of investment, and  
production of abundant radical species [1]–[5]. One of CAP  
sources is jet type, which can generate plasmas in open space  
rather than in confined discharge gaps and is characterized by  
flexibility, compact, and efficiency [6]–[9]. A promising CAP  
jet device for applications is the plasma needle with a single-  
electrode configuration, which makes it possible for direct  
treatments that have no limitation on the size of the objects to be  
treated [10]–[15]. However, for most of the plasma jet devices,  
the plasma jets cover only a few square millimeters, which  
make them difficult for large-scale applications, such as surface  
coating, deposition, cleaning, and medicine. One way to meet  
Manuscript received August 6, 2011; revised October 28, 2011; accepted  
March 8, 2012. Date of publication April 9, 2012; date of current version  
June 6, 2012. This work was supported by the National Natural Science  
Foundation of China under Grants 51077008 and 11175037.  
The authors are with the Center for the Plasma Science and Engineering,  
School of Physics and Optoelectronic Technology, Dalian University of Tech-  
nology, Dalian 116024, China (e-mail: ; qmy198502@  
eyou.com; ; ; ).  
Color versions of one or more of the figures in this paper are available online  
at http://ieeexplore.ieee.org.  
II. EXPERIMENTAL SETUP  
The 2-D CAP jet array considered in this study is shown  
schematically in Fig. 1, with a honeycomb configuration show-  
ing its structural details with both side and end views. As  
Digital Object Identifier 10.1109/TPS.2012.2191307  
0093-3813/$31.00 © 2012 IEEE  

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