Transition of a diffuse discharge to a spark at nanosecond breakdown of high-pressure nitrogen and air in a nonuniform electric field

2013 ◽  
Vol 58 (8) ◽  
pp. 1115-1121 ◽  
Author(s):  
V. F. Tarasenko ◽  
E. Kh. Baksht ◽  
M. I. Lomaev ◽  
D. V. Rybka ◽  
D. A. Sorokin
2011 ◽  
Vol 39 (11) ◽  
pp. 2088-2089 ◽  
Author(s):  
Mikhail I. Lomaev ◽  
Victor F. Tarasenko ◽  
Dmitri A. Sorokin ◽  
Dmitri V. Rybka

2008 ◽  
Vol 53 (7) ◽  
pp. 858-865 ◽  
Author(s):  
A. G. Rep’ev ◽  
P. B. Repin ◽  
E. G. Danchenko

2004 ◽  
Vol 34 (11) ◽  
pp. 1007-1010 ◽  
Author(s):  
S B Alekseev ◽  
V P Gubanov ◽  
I D Kostyrya ◽  
Viktor M Orlovskii ◽  
V S Skakun ◽  
...  

2010 ◽  
Vol 55 (2) ◽  
pp. 210-218 ◽  
Author(s):  
V. F. Tarasenko ◽  
E. Kh. Baksht ◽  
A. G. Burachenko ◽  
I. D. Kostyrya ◽  
M. I. Lomaev ◽  
...  

JETP Letters ◽  
2017 ◽  
Vol 106 (10) ◽  
pp. 653-658 ◽  
Author(s):  
D. V. Beloplotov ◽  
V. F. Tarasenko ◽  
D. A. Sorokin ◽  
M. I. Lomaev

2013 ◽  
Vol 58 (3) ◽  
pp. 370-374 ◽  
Author(s):  
A. M. Boichenko ◽  
V. F. Tarasenko ◽  
E. Kh. Baksht ◽  
A. G. Burachenko ◽  
M. V. Erofeev ◽  
...  

2013 ◽  
Vol 818 ◽  
pp. 72-76 ◽  
Author(s):  
Gang Su

The crystalline electric field parameters Anmfor HoFe11Ti under different pressures were evaluated by fitting calculations to the magnetization curves measured on the single crystals at several temperatures. It was found that magneto-crystalline anisotropy has been changed by high pressure and the Anmfor HoFe11Ti under high pressures are strikingly different from Anmfor the corresponding HoFe11Ti H with interstitial hydrogen atom.


2001 ◽  
Vol 700 ◽  
Author(s):  
Malinda M. Tupper ◽  
Marjorie E. Chopinaud ◽  
Takamichi Ogawa ◽  
Michael J. Cima

AbstractDispensing micron-scale dielectric materials can be achieved through the use of dielectrophoresis. Electrodes are designed to create a nonuniform electric field. This method is expected to be applicable for transfer of a wide range of dielectric powders as well as small, shaped components. Small, 150 μm diameter silica spheres, as well as sodium fluorescein powder have been dispensed by this method. Selecting the appropriate electrode geometry and electric field intensity controls the amount collected. As little as 1.0 μg of sodium fluorescein powder, and as much as 16 mg of silica beads have been collected, and repeatability within 10 % of the total amount dispensed has been achieved.


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