A computational discharge model for sphere–plane long air gap under switching impulse voltage
Source abstract
Abstract
There are lots of sphere–plane air gaps in valve halls in extra-high-voltage and ultra-high-voltage converter stations. Accurate prediction for discharge characteristics of sphere–plane gaps is of great significance for the selection of shielding structure and determining the dielectric strength of the valve hall. In this paper, based on the physical process of corona inception and continuous leader inception, a computational model for calculating the discharge voltage of a sphere–plane air gap under positive switching impulse voltage is proposed, and the leader characteristics and discharge voltage are analyzed. Then, the switching impulse discharge test of the sphere–plane gap with 0.15, 2, and 0.3 m radius spherical electrodes is carried out to verify the correctness of the model. The results show that the discharge voltage calculated by the proposed method is consistent with the test results, and the error is within 7.3%. The leader inception voltage and inception time increase with the increasing spherical electrode radius at the same gap distance, and an identical spherical electrode require higher leader inception voltage and faster leader inception time with the increasing gap distance.
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Research context
OpenAlex topics: High voltage insulation and dielectric phenomena · Aerosol Filtration and Electrostatic Precipitation · Lightning and Electromagnetic Phenomena
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Hubei Engineering Research Center for Safety Monitoring of New Energy and Power Grid Equipment, Hubei University of Technology 1 , Wuhan 430068, China
Electric Power Research Institute, China Southern Power Grid 2 , Guangzhou 510663, China
Funding
National Engineering Laboratory for Ultra High Voltage Engineering Technology
References (23)
Show source-provided references
1. Study of sphere-plate gap discharge characteristics and values for ±1100 kV EHV DC converter station10.13334/j.0258-8013.pcsee.200305 ↗
2. Streamer-to-leader transition in a sphere-to-plane air gap tested with switching impulses
3. Positive leaders propagate slower at higher altitudes: Experimental evidence and theoretical explanation10.1029/2021gl095995 ↗
4. Numerical modeling of electrical discharges in long air gaps tested with positive switching impulses10.1109/TPS.2018.2802039 ↗
5. Switching surge strength of large air gaps: A physical approach10.1109/t-pas.1976.32131 ↗
6. Switching impulse strength of air insulation: Leader inception criterion10.1109/61.35646 ↗
7. Fundamental processes in long air gap discharges10.1016/s1631-0705(02)01414-7 ↗
8. A simplified model for the simulation of positive-spark development in long air gaps10.1088/0022-3727/30/17/010 ↗
9. A simplified physical model to determine the lightning upward connecting leader inception10.1109/tpwrd.2005.859290 ↗
10. Unstable leader inception criteria of atmospheric discharges10.3390/atmos8090156 ↗
11. Observation of leader development in rod–rod air gaps under negative switching impulse10.7567/jjap.52.090206 ↗
12. The effect of corona discharge on leader initiation in long air gaps10.1109/tps.2014.2305446 ↗
13. Switching impulse breakdown characteristics of large sphere-plane air gaps compared with rod-plane air gap10.1109/tdei.2013.6518953 ↗
14. Comparative study of AC and positive and negative DC visual corona for sphere-plane gaps in atmospheric air10.3390/en11102671 ↗
15. A model for switching impulse leader inception and breakdown of long air-gaps10.1109/61.19251 ↗
16. Positive discharges in long air gap discharges results and conclusions
17. Positive corona inception voltages and corona currents for air at various pressures and humidities10.1109/tdei.2010.5412003 ↗
18. Calculation method for negative DC onset corona voltage in rod-plane gaps10.13334/j.0258-8013.pcsee.2016.08.032 ↗
19. Current–voltage characteristics of corona in rod–plane gaps as influenced by temperature10.1049/ip-smt:20030019 ↗
20. Corona-induced pressures, potentials, fields and currents in electrostatic precipitator configurations10.1088/0022-3727/40/7/014 ↗
21. Calculation of corona onset voltage for duct-type precipitators10.1109/28.216532 ↗
22. 2016
23. 2010