Impulse partial discharge and breakdown mechanism under non-uniform electric field in N/sub 2//SF/sub 6/ gas mixtures

Author(s):  
Y. Yoshitake ◽  
N. Hayakawa ◽  
T. Ueda ◽  
H. Okubo
Energies ◽  
2021 ◽  
Vol 14 (4) ◽  
pp. 1065
Author(s):  
Houssem Eddine Nechmi ◽  
Michail Michelarakis ◽  
Abderrahmane (Manu) Haddad ◽  
Gordon Wilson

Negative and positive partial discharge inception voltages and breakdown measurements are reported in a needle-plane electrode system as a function of pressure under AC voltage for natural gases (N2, CO2, and O2/CO2), pure NovecTM gases (C4F7N and C5F10O) and NovecTM in different natural gas admixtures. For compressed 4% C4F7N–96% CO2 and 6% C5F10O–12% O2–82% CO2 gas mixtures, the positive-streamer mode is identified as the breakdown mechanism. Breakdown and negative partial discharge inception voltages of 6% C5F10O–12% O2–82% CO2 are higher than those of 4% C4F7N–96% CO2. At 8.8 bar abs, the breakdown voltage of 6% C5F10O–12% O2–82% CO2 is equal to that of 12.77% O2–87.23% CO2 (buffer gas). Synergism in negative partial discharge inception voltage/electric field fits with the mean value and the sum of each partial pressure individually component for a 20% C4F7N–80% CO2 and 6% C5F10O–12% O2–82% CO2, respectively. In 9% C4F7N–91% CO2, the comparison of partial discharge inception electric fields is Emax (CO2) = Emax(C4F7N), and Emax (12.77% O2–87.23% CO2) = Emax(C5F10O) in 19% C5F10O–81%(12.77% O2–87.23% CO2). Polarity reversal occurs under AC voltage when the breakdown polarity changes from negative to positive cycle. Polarity reversal electric field EPR was quantified. Fitting results show that EPR (CO2) = EPR(9% C4F7N–91% CO2) and EPR(SF6) = EPR (22% C4F7N–78% CO2). EPR (4% C4F7N–96% CO2) = EPR (12.77% O2–87.23% CO2) and EPR (6% C5F10O–12% O2–82% CO2) < EPR (4% C4F7N–96% CO2) < EPR (CO2).


2018 ◽  
Vol 25 (4) ◽  
pp. 1371-1379 ◽  
Author(s):  
Ruishuang Zhong ◽  
Su Zhao ◽  
Xiaoling Zhao ◽  
Peng Xue ◽  
Juntao Jiao ◽  
...  

2020 ◽  
Vol 27 (4) ◽  
pp. 1119-1127
Author(s):  
Shenyang Mo ◽  
Zhibin Zhao ◽  
Xuebao Li ◽  
Xiang Cui ◽  
Jiayu Xu ◽  
...  

2011 ◽  
Vol 5 (2) ◽  
pp. 59-66 ◽  
Author(s):  
B. Florkowska ◽  
P. Zydron ◽  
M. Florkowski ◽  
J. Roehrich

2018 ◽  
Vol 25 (4) ◽  
pp. 1393-1402 ◽  
Author(s):  
Can Guo ◽  
Qiaogen Zhang ◽  
Jingtan Ma ◽  
Lingli Zhang ◽  
Yuan Li ◽  
...  

Energies ◽  
2020 ◽  
Vol 13 (11) ◽  
pp. 2676 ◽  
Author(s):  
Marek Florkowski ◽  
Dariusz Krześniak ◽  
Maciej Kuniewski ◽  
Paweł Zydroń

This paper describes a correlation of partial discharge phase-resolved patterns with an optical imaging performed in a non-uniform electric field configuration. The influence of different dielectric barrier materials, placed on the plane electrode, on the discharge propagation and surface landing was investigated. The investigations were focused on the corona at positive polarity of AC high voltage. It was found that the initial positive corona stage is similar for all cases whereas the discharge propagation and surface landing strongly depends on the barrier material properties. The observed streamer discharge modes have been described by the geometrical measures such as stem length, stretch of a discharge profile on the dielectric barrier surface and an hemispherical envelope of discharge filaments. Since various dielectrics reveal different properties of charge accumulation and surface neutralization, the charge memory effect may be visible and can be related to the ability to create and sustain of additional electric field component. It may refer to subsequent discharges as well as to conditions faced at the voltage polarity reversal. The correspondence between different forms of phase-resolved patterns have been associated with the modes of streamer discharges observed by optical imaging. Presented methodology poses huge potential for both scientific investigations on underlying discharge phenomena as well as on the application in future diagnostic systems of HV insulation.


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