Gas breakdown in an atmospheric pressure radio-frequency capacitive plasma source

2001 ◽  
Vol 89 (1) ◽  
pp. 15-19 ◽  
Author(s):  
Jaeyoung Park ◽  
I. Henins ◽  
H. W. Herrmann ◽  
G. S. Selwyn
2015 ◽  
Vol 15 (3) ◽  
pp. 2192-2196 ◽  
Author(s):  
Giichiro Uchida ◽  
Kosuke Takenaka ◽  
Atsushi Miyazaki ◽  
Yuichi Setsuhara

2021 ◽  
Vol 11 (18) ◽  
pp. 8430
Author(s):  
Sen Li ◽  
Jiazhen Sun ◽  
Rui Sun ◽  
Jie Pan ◽  
Lin Wang ◽  
...  

In this paper, argon was used in radio frequency (13.56 MHz) dielectric barrier discharge (rf-DBD) at atmospheric pressure. The IV curve was recorded after gas breakdown, and discharge photos were captured by ICCD camera. Discharges of α mode and γ mode were observed based on IV curve and ICCD photos. As the existence of negative glow in γ mode, the luminescence intensity of different position of the discharge gap was analyzed. It was found that in the α mode, the electron avalanche occurs from negative to positive and negative glow appeared after the discharge changed into γ mode. In every half cycle, the peak position of negative glow is 13 ± 1 ns later than that of electron avalanche on cathode surface.


2015 ◽  
Vol 107 (5) ◽  
pp. 053702 ◽  
Author(s):  
Xiaolong Deng ◽  
Anton Yu Nikiforov ◽  
Eusebiu-Rosini Ionita ◽  
Gheorghe Dinescu ◽  
Christophe Leys

2014 ◽  
Vol 21 (5) ◽  
pp. 053505 ◽  
Author(s):  
W. G. Huo ◽  
S. J. Jian ◽  
J. Yao ◽  
Z. F. Ding

2013 ◽  
Vol 15 (7) ◽  
pp. 623-626
Author(s):  
Xinkun Liu ◽  
Jinzhou Xu ◽  
Tongfei Cui ◽  
Ying Guo ◽  
Jing Zhang ◽  
...  

Author(s):  
Lei Wang ◽  
Constantinos Lazarou ◽  
Charalambos Anastassiou ◽  
George Elia Georghiou ◽  
Christophe Leys ◽  
...  

2001 ◽  
Vol 89 (1) ◽  
pp. 20-28 ◽  
Author(s):  
Jaeyoung Park ◽  
I. Henins ◽  
H. W. Herrmann ◽  
G. S. Selwyn ◽  
R. F. Hicks

Polymers ◽  
2021 ◽  
Vol 13 (13) ◽  
pp. 2132
Author(s):  
Ovidiu S. Stoican

A cold plasma source operating at atmospheric pressure powered by a voltage multiplier is reported. In addition to its usual high voltage output, there is an intermediate output of lower voltage and higher current capability. A discharge current is drawn from both outputs. The ratio of the current supplied by each output depends on the operating state, namely, before or after the plasma jet formation. The electrical circuit is equivalent to two dc sources connected in parallel, used to initiate and sustain the electrical discharge. The plasma source is aimed to study the effect of cold plasma on the surface of various liquid or solid materials, including polymers.


2020 ◽  
Vol 35 (10) ◽  
pp. 2369-2377
Author(s):  
Helmar Wiltsche ◽  
Matthias Wolfgang

The MICAP is a microwave driven plasma source employing nitrogen as the plasma gas. In this work we compare LODs and LOQs obtained in axial viewing with those obtained by ICP-OES and evaluate the effect of air instead of nitrogen as the plasma gas.


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