Improved Modeling of Hypersonic Weakly-Ionized Argon Plasma Flow

Author(s):  
Tarit Bose
1980 ◽  
Vol 23 (2) ◽  
pp. 271-282
Author(s):  
C. P. Schneider

Herein is described a calculation of the effective coffision frequency νeffof a low- density, shock-heated argon plasma under the influence of a weak electric field which oscillates harmonically with angular frequency ω. It is shown that, for the high frequency case ω >whereis the collision frequency in a Maxwellian gas plasma, one has νeff⋍ 2, provided that the imaginary part of the argon plasma conductivity is negligibly small in comparison to the real part. The influence of the theoretical model used to calculate νeffon the values of the electron temperatureTederived from measurements is compared with the results obtained in a data reduction for which the hard-sphere model for particle encounters was utilized.


2013 ◽  
Vol 34 (3) ◽  
pp. 559-577 ◽  
Author(s):  
Hai-Xing Wang ◽  
Wei-Ping Sun ◽  
Su-Rong Sun ◽  
A. B. Murphy ◽  
Yiguang Ju

2020 ◽  
Vol 2020.58 (0) ◽  
pp. 05c3
Author(s):  
Daichi SHIMIZU ◽  
Yasunori NAGATA ◽  
Toshinori KOUCHI ◽  
Shinichiro YANASE ◽  
Takumi NORII

Author(s):  
Andreas Knapp ◽  
Daniel Haag ◽  
Norifumi Ono ◽  
Markus Fertig ◽  
Georg Herdrich ◽  
...  

1972 ◽  
Vol 8 (2) ◽  
pp. 143-158 ◽  
Author(s):  
D. S. Bugnolo

The results of two experiments in a weakly ionized turbulent argon plasma are compared with a theory for the spacewisespectrum of the electron – ion density fluctuations of the plasma. It would appear that the theoretical predictions are in reasonable agreement with the results of these experiments. The theory, based on a quasi-static formulation of the Boltzmann equations, is a direct consequence of the Boltzman equations for the electrons, ions and neutrals in theweakly ionized plasma. A Heisenberg model is used for the turbulent diffusion coefficient of the plasma.


1985 ◽  
Vol 5 (1) ◽  
pp. 39-54 ◽  
Author(s):  
Masakazu Kobayashi ◽  
Takuya Honda ◽  
Atsushi Kanzawa

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