ARC-Circuit Interaction Near Current Zero and Circuit-Breaker Testing

1972 ◽  
Vol PAS-91 (3) ◽  
pp. 705-713 ◽  
Author(s):  
Werner Rieder
Keyword(s):  
2005 ◽  
Vol 33 (5) ◽  
pp. 1589-1593 ◽  
Author(s):  
E.P.A. van Lanen ◽  
M. Popov ◽  
L. van der Sluis ◽  
R.P.P. Smeets

2017 ◽  
Vol 4 (3) ◽  
pp. 234-240 ◽  
Author(s):  
Y. Guo ◽  
H. Zhang ◽  
Y. Yao ◽  
Q. Zhang ◽  
J. D. Yan

A high voltage gas blast circuit breaker relies on the high speed gas flow in a nozzle to remove the energy due to Ohmic heating at high current and to provide strong arc cooling during the current zero period to interrupt a fault current. The physical mechanisms that are responsible for the hugely different arc cooling capabilities of two gases (SF<sub>6</sub> and air) are studied in the present work and important gas material properties controlling the cooling strength identified.


2011 ◽  
Vol 39 (6) ◽  
pp. 1349-1353 ◽  
Author(s):  
Anton V. Schneider ◽  
Sergey A. Popov ◽  
Alexander V. Batrakov ◽  
Gabriela Sandolache ◽  
Stephen William Rowe

Author(s):  
Ralf Methling ◽  
Nicolas Götte ◽  
Dirk Uhrlandt

Molecule radiation can be used as a tool to study colder regions in switching arc plasmas like arc fringes in contact to walls and ranges around current zero (CZ). This is demonstrated in the present study for the first time for the case of ablation-dominated high&ndash;current arcs as key elements of self&ndash;blast circuit breakers. The arc in a model circuit breaker (MCB) in CO2 with and an arc in a long nozzle under ambient conditions with peak currents between 5 and 10 kA were studied by emission and absorption spectroscopy in the visible spectral range. The nozzle material was polytetrafluoroethylene (PTFE) in both cases. Imaging spectroscopy was carried out either with high-speed cameras or with intensified CCD cameras. A pulsed high-intensity Xe lamp was applied as background radiator for the broad-band absorption spectroscopy. Emission of Swan bands from carbon dimers was observed at the edge of nozzles only or across the whole nozzle radius with highest intensity in the arc center, depending on current and nozzle geometry. Furthermore, absorption of C2 Swan bands and CuF bands were found with the arc plasma serving as background radiator. After CZ, only CuF was detected in absorption experiments.


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