Measurement of the Neutral Copper Vapor Density around Current Zero of a 500-A Vacuum Arc Using Laser-Induced Fluorescence

1985 ◽  
Vol 13 (6) ◽  
pp. 577-581 ◽  
Author(s):  
G. Lins
2004 ◽  
Vol 124 (11) ◽  
pp. 945-953 ◽  
Author(s):  
Shinji Takahashi ◽  
Kazuyoshi Arai ◽  
Osami Morimiya ◽  
Kazuo Hayashi ◽  
Etsuo Noda

2020 ◽  
Vol 53 (30) ◽  
pp. 305201 ◽  
Author(s):  
Yuki Inada ◽  
Ryo Kikuchi ◽  
Hiroyuki Nagai ◽  
Akiko Kumada ◽  
Kunihiko Hidaka ◽  
...  

1997 ◽  
Vol 25 (4) ◽  
pp. 598-602 ◽  
Author(s):  
K. Koyama ◽  
Y. Nakayama ◽  
T. Ohi ◽  
K. Horinouchi ◽  
H. Sasao

2017 ◽  
Vol 45 (1) ◽  
pp. 129-139 ◽  
Author(s):  
Yuki Inada ◽  
Tomoki Kamiya ◽  
Shigeyasu Matsuoka ◽  
Akiko Kumada ◽  
Hisatoshi Ikeda ◽  
...  

2017 ◽  
Vol 4 (3) ◽  
pp. 249-252
Author(s):  
A. Khakpour ◽  
R. Methling ◽  
St. Franke ◽  
S. Gortschakow ◽  
D. Uhrlandt

A vacuum interrupter reaches its interruption limit once high-current anode phenomena occur. High-current anode modes lead to an increase of the anode surface temperature and an increased generation of metal vapor, which may result in a weakening of the dielectric recovery strength after current zero. In this work, different discharge modes in a vacuum arc for AC 50 Hz including diffuse, footpoint, anode spot type 1 and type 2, and anode plume are investigated. Electrodes made of CuCr7525 with diameter of 10 mm are used. The final gap length is about 20 mm. Time and space resolved optical emission spectroscopy is used to examine the temporal and spatial distribution of atomic and ionic copper lines. The distribution of atomic and ionic lines parallel and perpendicular to the anode surface is investigated. Radiator density is also determined for CuI, CuII, and CuIII near the anode surface.


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