2018
DOI: 10.1016/j.physa.2017.11.151
|View full text |Cite
|
Sign up to set email alerts
|

Kinetic theory of two-temperature polyatomic plasmas

Abstract: We investigate the kinetic theory of two-temperature plasmas for reactive polyatomic gas mixtures. The Knudsen number is taken proportional to the square root of the mass ratio between electrons and heavy-species, and thermal non-equilibrium between electrons and heavy species is allowed. The kinetic non-equilibrium framework also requires a weak coupling between electrons and internal energy modes of heavy species. The zeroth-order and first-order fluid equations are derived by using a generalized Chapman-Ens… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
6
0

Year Published

2019
2019
2024
2024

Publication Types

Select...
6
2

Relationship

2
6

Authors

Journals

citations
Cited by 8 publications
(6 citation statements)
references
References 34 publications
0
6
0
Order By: Relevance
“…This justifies the need to derive a multicomponent diffusion model for reacting gases and nanoparticles mixtures. This can be done by extending existing methods from kinetic theory [65].…”
Section: Discussionmentioning
confidence: 99%
“…This justifies the need to derive a multicomponent diffusion model for reacting gases and nanoparticles mixtures. This can be done by extending existing methods from kinetic theory [65].…”
Section: Discussionmentioning
confidence: 99%
“…When the Knudsen number is small enough to use the Chapman-Enskog method, the transport fluxes are shown to be linearly proportional to transport forces. For instance, neglecting thermal diffusion, the diffusion velocities are modeled by means of the generalized Fick law, V i = − j∈S D ij d j , i ∈ S. The diffusion force is d i = (∇P i − n i q i E)/P , with the partial pressure P i , number density n i , and charge q i of species i ∈ S, and the electric field E. 45 In this case, the calculation of the species velocity distribution function is no longer required, since the multicomponent diffusion coefficients D ij , i, j ∈ S, have a closed form in terms of average cross-sections based on binary interaction potentials between the species pairs. 43 Electrons and heavy particles can exhibit distinct temperatures due to their mass disparity.…”
Section: Maxwell Transfer Equations and Nonequilibrium Modelsmentioning
confidence: 99%
“…The starting point for plasma gas mixtures is given in the following reference frame, see also [10], [11] and [17]. We concentrate on the heavy particle description, which is discussed in [18].…”
Section: Mathematical Modelmentioning
confidence: 99%