Abstract

Numerical solution of the Boltzmann equation for stationary high-speed flows around complex three-dimensional bodies is an extremely difficult computational problem. This is because of high dimension of the equation and lack of efficient implicit methods for the calculation of the collision integral on arbitrary non-uniform velocity grids. Therefore, the use of the so-called model (approximate) kinetic equations appears to be more appropriate and attractive. This article uses the numerical methodology recently developed by the second author which includes an implicit method for solving the approximating kinetic equation of E.M. Shakhov (S-model) on arbitrary unstructured grids in both velocity and physical spaces. Since most of model equations have a well-known drawback associated with the velocityindependent collision frequency it is important to determine the deviations of solutions of these equations from the solution of the complete Boltzmann equation or DSMC for high-speed gas flows. Our recent comparison of the DSMC and S-model solutions for monatomic gases with a soft interaction potential shows good agreement of surface coefficients of the pressure, heat transfer and friction, which are most important for industrial applications. In this paper, we compare the solution of model equations and the Boltzmann equation for the problem of supersonic gas flow around a cylinder when molecules interact according to the law of hard spheres. Since this law of molecular interaction is the most rigid, the difference in solutions can show the maximum error that can be obtained by using model equations instead of the exact Boltzmann equation in such problems. Our high-fidelity computations show that the use of model kinetic equations with adaptation in phase space is very promising for industrial applications.

Highlights

  • At present there is a large number of studies devoted to the analysis of highly non-equilibrium external rarefied gas flows at high-speed (M∞ ≥ 10) regimes

  • Calculations presented in [8] demonstrate that the pressure, friction and heat transfer coefficients on the surface of the body in case of monatomic gas at super- and high-speed flow regimes are very close to the direct simulation Monte-Carlo (DSMC) results for the S-model kinetic equation of E.M

  • The second computation package used in the present study is the kinetic module of the Unifed Flow Solver (UFS) [2] which can solve both BKE and model kinetic equations

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Summary

Introduction

At present there is a large number of studies devoted to the analysis of highly non-equilibrium external rarefied gas flows at high-speed (M∞ ≥ 10) regimes. Since for high-speed flows over convex body there appears strong non-equilibrium boundary layer, it is important to use the so-called kinetic approaches in the analysis. This class of flows requires the use of considerable computing resources in case of three-dimensional geometries if one uses the direct simulation Monte-Carlo methods Since such a viscosity law is the most “rigid”, the difference between solutions will show the maximum possible error which can occur due to the usage of the model kinetic equations instead of BKE

Formulation of the Problem and Governing Equations
Kinetic Solvers and Details of the Calculations
Results
Conclusions
Full Text
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