Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

O5.302 Self--consistent modeling of Discharge: the role of superelastic collisions

Jul 6, 2018, 11:55 AM
15m
Mánes Bar

Mánes Bar

Talk LTDP

Speaker

Gianpiero Colonna

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See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/O5.302.pdf Self–consistent modeling of Discharge: the role of superelastic collisions G. Colonna PLASMI Lab NANOTEC CNR Bari (Italy) To determine the rate coefficients of electron-induced processes the Boltzmann equation for free electrons must be solved to calculate the electron energy distribution function (eedf). Inte- grating the cross sections over the eedf, the rates of electron induced processes are calculated. The most advanced approach consists in coupling self–consistently the Boltzmann equation, with the state-to-state kinetics, determining at the same time the eedf and the level distribu- tion, accounting for their mutual interaction. To simplify the calculation, under the assump- tion that eedf relaxes much faster than the gas composition, the rate coefficients can be related only to the local electric field (local field approximation, LFA). However, LFA cannot consider the contribution of the superelastic collisions in the electron kinetics. In participating to the Round Robin [1] activity for the verification of different plasma kinetic codes, strong effects of superelastic collisions on the plasma prop- !2 erties have been observed, when a self– 1014 P = t e t/t0 P0 t0 Ar* consistent coupling of free electron and level 1011 P0 = 10 W particle density [cm-3] cm3 kinetics has been considered. It is well known t0 = 10 3 s 108 e- that superelastic collisions are very important 105 in the post-discharge. In the present work we Ar* e- 102 have observed that they are effective also in 10–1 the presence of high electric field, as shown in 10–10 10–8 10–6 10–4 10–2 100 time [s] the figure, where the density of free electrons and argon metastable are reported when su- Figure 1: Electron and argon metastable densities perelastic collisions are neglected or included with (continuous lines) and without (dashed lines) superelastic collisions in the Boltzmann equation. in the Boltzmann equation. When superelas- tic collisions are considered in the electron ki- netics, some plateaux appear in the eedf [2, 3], which completely change the rates of electron induced processes. These rates depends not only on the electric field, but also on the level pop- ulation and on the plasma composition, affecting the time evolution of species densities. References [1] L. Pitchford et al.: Plasma chemistry round robin, GT1.00063, 70th Annual GEC, 2017. [2] G. Colonna, A. D’Angola (Ed), Plasma Modeling: Methods and Applications, IOP (2017) [3] M: Capitelli et. al, Fundamental Aspects of Plasma Chemical-Physics: Kinetics (2016)

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