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A New Modified Pseudoequilibrium Calculation to Determine the Composition of Hydrogen and Nitrogen Plasmas at Atmospheric Pressure
Authors:P. André  J. Aubreton  M. F. Elchinger  P. Fauchais  A. Lefort
Affiliation:(1) LAEPT, CNRS URA 828, Université Blaise Pascal, 24, Avenue des Landais, 63117 Aubière Cedex, France;(2) SPCTS, CNRS UMR 6638, Université de Limoges, 123, Avenue Albert Thomas, 87060 Limoges Cedex, France
Abstract:This paper proposes a modified pseudoequilibrium calculation, which gives almost the same results as those of kinetic calculations to determine the composition of hydrogen and nitrogen plasmas at atmospheric pressure. The computing time is two to three orders of magnitude faster than that of the kinetic calculations. First, according to experimental results, a relationship between the electron temperature Te and the heavy species one Th has been proposed. The ratio Te/Th varies as a function of the logarithm of the ratio ne/nemax, emax being the electron density in the plasma core for which equilibrium is achievedemax ~ 1023 ). The kinetic calculations have been performed assuming the microreversibility where the backward kinetic rate coefficient kb is calculated by kd/kb=Kx, where kd is the direct kinetic coefficient and Kx the molar fraction equilibrium constant. When electrons are involved in both direct and backward reactions, kd and Kx are expressed as functions of Te . However, when the direct reaction involves electrons while the backward one is due to collisions between heavy species (or the reverse), a temperature T* between Te and Th is introduced. T* is determined as a function of the ratio of the electron flux to that of neutral species in such a way that T*=Tefor ne > 1023 and T*=Th for low values of ne(ne < 1015 m–3). Compared to hydrogen, the nitrogen composition exhibits a very abrupt variation between 6000 and 6500 K, corresponding to a shift from the dissociation-dominated regime to that of ionization. It occurs because dissociation of nitrogen starts almost simultaneously with its ionization, which is not the case of H2, for which dissociation is terminated long before ionization starts. If the charge transfer reaction, whose activation energy is low for both gases, is neglected, in both cases the electron density increases drastically below 9000 K. These results are quite similar to those obtained when calculating the composition with the multitemperature mass action law. The kinetic calculations are dominated by the reactions with a low activation energy: dissociation, dissociative recombination and charge transfer. Thus, a modified pseudoequilibrium calculation has been introduced, the plasma composition being calculated with the equilibrium constants corresponding to low activation energies[X2 rarr 2X, e+X2+ rarr 2X, X2++X rarr X+ + X2 both for hydrogen (X=H) and nitrogen (X=N)] at the temperature T* between Te and Th. The results are in very good agreement with those of the kinetic calculations.
Keywords:multitemperature thermal plasmas  composition of hydrogen and nitrogen plasmas  kinetic calculations  pseudoequilibrium calculations
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