scholarly journals Kinetic simulation of a low-pressure helium discharge with comparison to experimental measurements

2019 ◽  
Vol 28 (5) ◽  
pp. 055012 ◽  
Author(s):  
Andrew Fierro ◽  
Ed Barnat ◽  
Chris Moore ◽  
Matthew Hopkins ◽  
Paul Clem
2021 ◽  
pp. 207-211
Author(s):  
V.S. Boldasov ◽  
A.I. Kuzmichev ◽  
M.S. Melnichenko ◽  
V.M. Shulaev

The kinetic simulation of high-voltage beam discharge at low pressure of nitrogen is fulfilled. The characteristics of particle flows to the tantalum cathode and back reflection of fast nitrogen atoms are calculated. The reflection coefficient equals tens of percents at voltages up to 100 kV. The generation of fast nitrogen atoms may be used for metals and dielectrics nitriding with implantation effect.


2020 ◽  
Vol 320 ◽  
pp. 00020
Author(s):  
Vitaliy Skvortsov ◽  
Vladimir B. Tupov

Gas distribution points (GDP) at TPPs are sources of intense noise. Results of noise experimental measurements originating from TPP GDP demonstrate that the sound level at a distance of 10 m could reach 110 dBA. Gas reduction valves are the source of noise in GDP. Noise emission characteristic of the gas reduction valves depends on their geometric and design parameters. To reduce the noise propagating in a low-pressure gas pipeline from gas reduction valves, various types of noise silencers are used. This paper presents results of noise experimental measurements in the vicinity of the GDP buildings at various energy enterprises. Overview and classification of silencers by various manufacturers used at TPP GDPs are provided.


1978 ◽  
Vol 33 (11) ◽  
pp. 1285-1293
Author(s):  
H. W. Drawin ◽  
J. Ramette

=The line profile of the HeI line at λ447.15 nm has been measured during the ionisation phase and during the afterglow of a condensed low-pressure helium discharge by means of a 10-channel spectrum analyzer having a channel width of 0.1 Å. The temporal resolution was I.6 μs (e-folding time). The filling pressure ranged from one to twenty Torr. The same relative peak structure was observed during the plasma build-up phase and the afterglow, only the intensities of the peaks were different in the two cases. Our measured profiles are quite similar to those obtained under different experimental conditions by other authors who explained the structure as being due to Baranger-Mozer plasma satellites. In contrast to this we did not find any correlation between electron density and peak position, i.e. the interpretation as Baranger- Mozer plasma satellites has to be excluded. The wavelengths of a number of peaks agree well with already identified He2 molecular lines, and there are sufficient experimental indications to conclude that the prominent part of the satellite structure originates from He0 molecular transitions most of which have not yet been identified.


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