Transport properties of ionized species
ABSTRACT: A universally applicable model is presented for the calculation of the transport properties of ionized species in CFD simulations. A multicomponent mixture formulation and simple mixing rules are used to compute the transport coefficients of dissociated and ionized air from room temperatu...
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| Main Authors: | , |
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| Format: | Article (Journal) |
| Language: | English |
| Published: |
December 1999
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| In: |
Annals of the New York Academy of Sciences
Year: 1999, Volume: 891, Pages: 72-80 |
| ISSN: | 1749-6632 |
| DOI: | 10.1111/j.1749-6632.1999.tb08754.x |
| Online Access: | Verlag, Volltext: http://dx.doi.org/10.1111/j.1749-6632.1999.tb08754.x Verlag, Volltext: http://onlinelibrary.wiley.com/doi/10.1111/j.1749-6632.1999.tb08754.x/abstract 
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| Author Notes: | Stefan Selle and Uwe Riedel, Interdisziplinäres Zentrum für Wissenschaftliches Rechnen, Universität Heidelberg |
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| 245 | 1 | 0 | |a Transport properties of ionized species |c Stefan Selle and Uwe Riedel, Interdisziplinäres Zentrum für Wissenschaftliches Rechnen, Universität Heidelberg |
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| 520 | |a ABSTRACT: A universally applicable model is presented for the calculation of the transport properties of ionized species in CFD simulations. A multicomponent mixture formulation and simple mixing rules are used to compute the transport coefficients of dissociated and ionized air from room temperature up to 30000 K at different pressures. Both formulations share little input data, which simplifies the handling of the transport model. The calculated binary diffusion coefficients are similar to the results of Levin et al.1-3 and Capitelli et al.4 The computed transport coefficients of the mixture are compared to the results of Gupta et al.5 A good agreement is found in the temperature range below 10000 K. At higher temperatures the results differ, because of the differences in the collision integrals of neutral-ion and Coulomb interactions and because of the use of higher approximations of transport properties of electrons in the present model. | ||
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