Neutral Atom Density at Current Zero in Interruption of Intense-Mode Vacuum Arc

Author(s):  
Ryo Kikuchi ◽  
Yuichi Hirano ◽  
Haruki Ejiri ◽  
Yuki Inada ◽  
Akiko Kumada ◽  
...  
1989 ◽  
Vol 17 (5) ◽  
pp. 666-671 ◽  
Author(s):  
E. Hayess ◽  
B. Juttner ◽  
G. Lieder ◽  
W. Neumann ◽  
H. Pursch ◽  
...  

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.


Author(s):  
Naoji Yamamoto ◽  
Masataka Iwamoto ◽  
Taichi Morita ◽  
Hideki Nakashima

1982 ◽  
Vol 36 (2) ◽  
pp. 168-171 ◽  
Author(s):  
P. K. Schenck ◽  
J. C. Travis ◽  
G. C. Turk ◽  
T. C. O'Haver

The temporal and spatial evolution of the depleted neutral atom density following laser-enhanced ionization in laminar flow flames has been used to characterize the flow velocity of the flame gases. This technique utilizes a low power cw dye laser and a low sodium seed density (1011 to 1012 atoms/ml). The flow velocity can be measured to better than 2% in standard analytical burners.


2013 ◽  
Vol 41 (8) ◽  
pp. 2022-2028 ◽  
Author(s):  
Anton V. Schneider ◽  
Sergey A. Popov ◽  
Alexander V. Batrakov ◽  
Gabriela Sandolache ◽  
Hans Schellekens

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