Xuan Zhou, She Chen, Hai Wang, 等. Experiment on leader propagation characteristics of air gaps in UHVDC transmission towers under positive switching impulse voltages[J]. 中国电机工程学会电力与能源系统学报(英文), 2015,1(3):42-48.
Xuan Zhou, She Chen, Hai Wang, et al. Experiment on leader propagation characteristics of air gaps in UHVDC transmission towers under positive switching impulse voltages[J]. CSEE Journal of Power and Energy Systems, 2015, 1(3): 42-48.
Xuan Zhou, She Chen, Hai Wang, 等. Experiment on leader propagation characteristics of air gaps in UHVDC transmission towers under positive switching impulse voltages[J]. 中国电机工程学会电力与能源系统学报(英文), 2015,1(3):42-48. DOI: 10.17775/CSEEJPES.2015.00034.
Xuan Zhou, She Chen, Hai Wang, et al. Experiment on leader propagation characteristics of air gaps in UHVDC transmission towers under positive switching impulse voltages[J]. CSEE Journal of Power and Energy Systems, 2015, 1(3): 42-48. DOI: 10.17775/CSEEJPES.2015.00034.
Experiment on leader propagation characteristics of air gaps in UHVDC transmission towers under positive switching impulse voltages
摘要
Abstract
Rapid developments in EHV/UHV transmission systems require a deeper understanding of the mechanism of long air gap discharge. Leader propagation is one of the main processes in long gap breakdown. In this paper
the leader propagation characteristics of real size ±800 kV UHVDC transmission tower gaps under positive switching impulse voltages (185/ 2290 μs) are investigated. An integrated observation platform consisting of an impulse voltage divider
a coaxial shunt
a high-speed video camera
and a set of integrated optical electric field sensors (IOES)
is established. The waveforms of impulse voltage
discharge current
electric field variation at specific positions
and time-resolved photographs of discharge morphology are recorded. Axial leader velocity and the relationship between leader advancements and injected charge are obtained. The typical value of leader stable propagation velocity is 1.7-2.2 cm/μs
which varies slightly with the gap length and applied voltage amplitude. The leader velocity in the re-illumination process is much higher
and is seen as varying from 5 cm/μs to 30 cm/μs
with an average value around 10 cm/μs. The charge in leader channel per unit length is 20- 40 μC/m
which illustrates a near-direct proportion relationship between discharge current and leader velocity. The observed parameters are important for further simulation of the tower gap breakdown processes.