Abstract

The calculation of the diffusion matrix in mixtures of dilute gases with large numbers (N) of components is revisited. An extremely simple relation providing the multicomponent diffusion matrix as a power series in terms of the N−1 independent mole fractions in the mixture is analytically derived from the kinetic theory of gases. This power series provides a convergent scheme with high convergence rate in the case of a gas mixture with one major component in which the remaining N−1 species are diluted. However, the convergence rate of this power series is lower if a certain number (M) of these species are far from the dilute limit. In that case we show that a straightforward modification of the former scheme leads to a relation providing the diffusion matrix as a power series in terms of a subset of N−1−M mole fractions, which are assumed to be dilute, keeping full dependence on the mole fractions of the remaining 1+Mmajor species. This relation takes full advantage of the usual situation found in combustion, where there is a relatively small number of major species (here 1+M), with the remaining N−1−M chemical components (often radicals) being in trace amounts. The error found in the diffusion fluxes with each one of these new methods in a typical combustion scenario is analyzed as a function of the number of terms included in the expansion. It is found that the second method (based on a power series in terms of the dilute species), truncated at the linear term, produces relative errors less than 1% in all the cases considered—including cases far from the dilute limit. Hence, this method provides an efficient tool for the accurate calculation of multicomponent diffusion fluxes in combustion.

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