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Glow Discharge in a High-Velocity Air Flow: The Role of the Associative Ionization Reactions Involving Excited Atoms
A kinetic scheme for non-equilibrium regimes of atmospheric pressure air discharges is developed. A distinctive feature of this model is that it includes associative ionization with the participation of N((2)D, (2)P) atoms. The thermal dissociation of vibrationally excited nitrogen molecules and the...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6721176/ https://www.ncbi.nlm.nih.gov/pubmed/31398836 http://dx.doi.org/10.3390/ma12162524 |
Sumario: | A kinetic scheme for non-equilibrium regimes of atmospheric pressure air discharges is developed. A distinctive feature of this model is that it includes associative ionization with the participation of N((2)D, (2)P) atoms. The thermal dissociation of vibrationally excited nitrogen molecules and the electronic excitation from all the vibrational levels of the nitrogen molecules are also accounted for. The model is used to simulate the parameters of a glow discharge ignited in a fast longitudinal flow of preheated (T(0) = 1800–2900 K) air. The results adequately describe the dependence of the electric field in the glow discharge on the initial gas temperature. For T(0) = 1800 K, a substantial acceleration in the ionization kinetics of the discharge is found at current densities larger than 3 A/cm(2), mainly due to the N((2)P) + O((3)P) → NO(+) + e process; being the N((2)P) atoms produced via quenching of N(2)(A(3)∑(u)(+)) molecules by N((4)S) atoms. Correspondingly, the reduced electric field noticeably falls because the electron energy (6.2 eV) required for the excitation of the N(2)(A(3)∑(u)(+)) state is considerably lower than the ionization energy (9.27 eV) of the NO molecules. For higher values of T(0), the associative ionization N((2)D) + O((3)P) → NO(+) + e process (with a low–activation barrier of 0.38 eV) becomes also important in the production of charged particles. The N((2)D) atoms being mainly produced via quenching of N(2)(A(3)∑(u)(+)) molecules by O((3)P) atoms. |
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