Numerical Comparison of Solutions of Kinetic Model Equations

The collision integral approximation by different model equations has created a whole new trend in the theory of rarefied gas. One widely used model is the Shakhov model (S-model) obtained by expansion of inverse collisions integral in a series of Hermite polynomials up to the third order. Using the...

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Main Author: A. A. Frolova
Format: Article
Language:Russian
Published: MGTU im. N.È. Baumana 2016-06-01
Series:Matematika i Matematičeskoe Modelirovanie
Subjects:
Online Access:https://www.mathmelpub.ru/jour/article/view/39
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spelling doaj-ee8795376d684e73bcb7026f2044ca7a2021-07-28T21:09:06ZrusMGTU im. N.È. BaumanaMatematika i Matematičeskoe Modelirovanie2412-59112016-06-0106617738Numerical Comparison of Solutions of Kinetic Model EquationsA. A. Frolova0Institution of Russian Academy of Sciences, Dorodnicyn Computing Centre of RASThe collision integral approximation by different model equations has created a whole new trend in the theory of rarefied gas. One widely used model is the Shakhov model (S-model) obtained by expansion of inverse collisions integral in a series of Hermite polynomials up to the third order. Using the same expansion with another value of free parameters leads to a linearized ellipsoidal statistical model (ESL).Both model equations (S and ESL) have the same properties, as they give the correct relaxation of non-equilibrium stress tensor components and heat flux vector, the correct Prandtl number at the transition to the hydrodynamic regime and do not guarantee the positivity of the distribution function.The article presents numerical comparison of solutions of Shakhov equation, ESL- model and full Boltzmann equation in the four Riemann problems for molecules of hard spheres.We have considered the expansion of two gas flows, contact discontinuity, the problem of the gas counter-flows and the problem of the shock wave structure. For the numerical solution of the kinetic equations the method of discrete ordinates is used.The comparison shows that solution has a weak sensitivity to the form of collision operator in the problem of expansions of two gas flows and results obtained by the model and the kinetic Boltzmann equations coincide.In the problem of the contact discontinuity the solution of model equations differs from full kinetic solutions at the point of the initial discontinuity. The non-equilibrium stress tensor has the maximum errors, the error of the heat flux is much smaller, and the ESL - model gives the exact value of the extremum of heat flux.In the problems of gas counter-flows and shock wave structure the model equations give significant distortion profiles of heat flux and non-equilibrium stress tensor components in front of the shock waves. This behavior is due to fact that in the models under consideration there is no dependency of the collision frequency on the molecular velocity.As calculations show, the ESL-model describes more accurately the non-equilibrium flow regime, but gives a greater deviation from the Boltzmann equation, than the Shahov model in front of shock waves.DOI: 10.7463/mathm.0615.0823537https://www.mathmelpub.ru/jour/article/view/39boltzmann equationmodel equationsthe equation of bgkellipsoidal statistical model (es)shakhov model (s-model)
collection DOAJ
language Russian
format Article
sources DOAJ
author A. A. Frolova
spellingShingle A. A. Frolova
Numerical Comparison of Solutions of Kinetic Model Equations
Matematika i Matematičeskoe Modelirovanie
boltzmann equation
model equations
the equation of bgk
ellipsoidal statistical model (es)
shakhov model (s-model)
author_facet A. A. Frolova
author_sort A. A. Frolova
title Numerical Comparison of Solutions of Kinetic Model Equations
title_short Numerical Comparison of Solutions of Kinetic Model Equations
title_full Numerical Comparison of Solutions of Kinetic Model Equations
title_fullStr Numerical Comparison of Solutions of Kinetic Model Equations
title_full_unstemmed Numerical Comparison of Solutions of Kinetic Model Equations
title_sort numerical comparison of solutions of kinetic model equations
publisher MGTU im. N.È. Baumana
series Matematika i Matematičeskoe Modelirovanie
issn 2412-5911
publishDate 2016-06-01
description The collision integral approximation by different model equations has created a whole new trend in the theory of rarefied gas. One widely used model is the Shakhov model (S-model) obtained by expansion of inverse collisions integral in a series of Hermite polynomials up to the third order. Using the same expansion with another value of free parameters leads to a linearized ellipsoidal statistical model (ESL).Both model equations (S and ESL) have the same properties, as they give the correct relaxation of non-equilibrium stress tensor components and heat flux vector, the correct Prandtl number at the transition to the hydrodynamic regime and do not guarantee the positivity of the distribution function.The article presents numerical comparison of solutions of Shakhov equation, ESL- model and full Boltzmann equation in the four Riemann problems for molecules of hard spheres.We have considered the expansion of two gas flows, contact discontinuity, the problem of the gas counter-flows and the problem of the shock wave structure. For the numerical solution of the kinetic equations the method of discrete ordinates is used.The comparison shows that solution has a weak sensitivity to the form of collision operator in the problem of expansions of two gas flows and results obtained by the model and the kinetic Boltzmann equations coincide.In the problem of the contact discontinuity the solution of model equations differs from full kinetic solutions at the point of the initial discontinuity. The non-equilibrium stress tensor has the maximum errors, the error of the heat flux is much smaller, and the ESL - model gives the exact value of the extremum of heat flux.In the problems of gas counter-flows and shock wave structure the model equations give significant distortion profiles of heat flux and non-equilibrium stress tensor components in front of the shock waves. This behavior is due to fact that in the models under consideration there is no dependency of the collision frequency on the molecular velocity.As calculations show, the ESL-model describes more accurately the non-equilibrium flow regime, but gives a greater deviation from the Boltzmann equation, than the Shahov model in front of shock waves.DOI: 10.7463/mathm.0615.0823537
topic boltzmann equation
model equations
the equation of bgk
ellipsoidal statistical model (es)
shakhov model (s-model)
url https://www.mathmelpub.ru/jour/article/view/39
work_keys_str_mv AT aafrolova numericalcomparisonofsolutionsofkineticmodelequations
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