Cathode Process in the KF-AlF3-Al2O3 Melts

2019 ◽  
Vol 166 (15) ◽  
pp. D784-D791 ◽  
Author(s):  
A. Yu. Nikolaev ◽  
A. V. Suzdaltsev ◽  
Yu. P. Zaikov
Keyword(s):  
1979 ◽  
Vol 40 (C7) ◽  
pp. C7-281-C7-282
Author(s):  
A. P. Kchuzeev ◽  
Yu. D. Korolev ◽  
V. A. Kuzmin ◽  
G. A. Mesyats ◽  
V. P. Rotshtein ◽  
...  

1992 ◽  
Vol 37 (2) ◽  
pp. 263-268 ◽  
Author(s):  
V.I. Taranenko ◽  
I.V. Zarutskii ◽  
V.I. Shapoval ◽  
M. Makyta ◽  
K. Matiašovský

2016 ◽  
Vol 75 (15) ◽  
pp. 69-78
Author(s):  
R. Abdulaziz ◽  
L. D. Brown ◽  
D. Inman ◽  
C. Sharrad ◽  
P. R. Shearing ◽  
...  

2012 ◽  
Vol 125-126 ◽  
pp. 29-33 ◽  
Author(s):  
Zhidong Liu ◽  
Xiaohua Yu ◽  
Gang Xie ◽  
Ying Lu ◽  
Yanqing Hou ◽  
...  

2006 ◽  
Vol 51 (26) ◽  
pp. 5825-5828
Author(s):  
M. Ambrová ◽  
V. Danielik ◽  
P. Fellner ◽  
J. Thonstad

2013 ◽  
Vol 12 (05) ◽  
pp. 1350037
Author(s):  
D. V. MATULKA ◽  
I. I. GRYGORCHAK ◽  
B. A. LUKIYANETS

Double-matrix hierarchical structure of the 〈molecular-lattice matrix MCM-41〈hydroquinone〉〉 is synthesized. Its use in the cathode process in the Li +-intercalation current generation showed a significant improvement in the structure of the discharge curve and the practical constancy of diffusion coefficient throughout the discharge process. Theoretical model describing the peculiarities of observed characteristics in the structure is presented.


The growth of pre-breakdown ionization currents I in uniform fields in nitrogen has been measured over a range of the spark parameters E/p from 41 to 45 V/cm/mm Hg and pd up to 810 mm Hg cm with sparking potentials up to 38 kV, where p is the gas pressure and d the electrode separation. The graphs of log I against d were initially linear, but at separations near the sparking distance the graphs curved upwards, indicating the existence of both primary α and secondary ( ω/α ) ionization mechanisms. The sparking potentials and distance here measured were found to be exactly in accordance with those predicted by the growth of current equation I = I 0 exp ( αd )/[1 – ( ω/α ) {exp( αd ) –1 }]. There were strong indications that the secondary ionization was, in fact, a cathode process. Possible effects of space charge were also considered, and the spark mechanism discussed.


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