2015
DOI: 10.1016/j.camwa.2015.04.028
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Comparison of relaxation phenomena in binary gas-mixtures of Maxwell molecules and hard spheres

Abstract: a b s t r a c tThe strategy for computing the Boltzmann collision integrals for gaseous mixtures is presented and bestowed to compute the fully non-linear Boltzmann collision integrals for hard sphere gas-mixtures. The Boltzmann collision integrals associated with the first 26 moments of each constituent in a gas-mixture are presented. Moreover, the Boltzmann collision integrals are exploited to study the relaxation phenomena of diffusion velocities, stresses and heat fluxes in binary gas-mixtures of Maxwell m… Show more

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Cited by 16 publications
(6 citation statements)
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“…For the above one-dimensional problem, the relevant boundary conditions associated with the 2×G13 equations are conditions (27)-(30) for each constituent while those associated with the 2×G26 equations are conditions (27), (28) and (31)-(33) for each constituent. Note that boundary conditions (29) and (31) for the problem under consideration just imply that the slip velocity vanishes, i.e, V = 0, and the other boundary conditions-for the problem under consideration-in linear-dimensionless form are as follows. Boundary conditions (27) and 28read…”
Section: Linear-dimensionless Boundary Conditionsmentioning
confidence: 99%
See 1 more Smart Citation
“…For the above one-dimensional problem, the relevant boundary conditions associated with the 2×G13 equations are conditions (27)-(30) for each constituent while those associated with the 2×G26 equations are conditions (27), (28) and (31)-(33) for each constituent. Note that boundary conditions (29) and (31) for the problem under consideration just imply that the slip velocity vanishes, i.e, V = 0, and the other boundary conditions-for the problem under consideration-in linear-dimensionless form are as follows. Boundary conditions (27) and 28read…”
Section: Linear-dimensionless Boundary Conditionsmentioning
confidence: 99%
“…Recently, the method has also been extended to single-component rarefied granular gases of hard spheres [25][26][27]. It is worth to note that the computation of full nonlinear production terms-the terms arising from the Boltzmann collision operator-associated with the moment equations derived in these works is not easy, and the present authors have also developed an automated way to compute them using computer algebra software Mathematica R , see [23,[28][29][30] for its details and [31] for the source code.…”
Section: Introductionmentioning
confidence: 99%
“…The details of the computation can be found in Gupta & Torrilhon (2012) and the source code for the computation is provided as supplementary material with the present paper. Interested readers are also referred to Gupta & Torrilhon (2015b); Gupta (2015) for deriving the higher-order moment equations for monatomic gas mixtures and to Gupta & Torrilhon (2015a); Gupta (2015) for learning the computation of their associated production terms, which might be useful in developing higher-order moment theories for granular gas mixtures. For the sake of completeness, we provide the production terms associated with the G26 equations (eqs.…”
Section: Grad 26-moment Closurementioning
confidence: 99%
“…It is well-known that the numerical methods for multi-species Boltzmann equations are computationally expensive (see for instance [30] and the references therein). On the other hand, BGK approximations are not able to reproduce peculiar nonlinear effects, especially in the evolution of high order moments in mixtures with heavy and light components [29]. This is also due to the fact that BGK operators do not include all the details of the different intermolecular potentials [50].…”
mentioning
confidence: 98%