Abstract:In this paper we incorporate a non-equilibrium thermodynamics perspective that is consistent with the Onsager reciprocity principle into the lattice Boltzmann framework to propose a novel regularized lattice Boltzmann formulation for modeling the Navier-Stokes-Fourier equations. The new method is applied to one-dimensional isothermal situations wherein the advantages of incorporating such a non-equilibrium perspective can be explicitly appreciated. In such situations, the non-equilibrium contribution of the la… Show more
“…Similarly, Xu (2003) solved the force-driven plane Poiseuille flow problem by employing the BGK–Burnett and the () BGK–super-Burnett schemes in the Boltzmann equations and demonstrated better results than those obtained using the N-S equations. An alternate way of solving the Boltzmann–BGK equation directly is through the lattice Boltzmann method (LBM) route; recent attempts to employ LBM schemes to solve high- flows have been detailed in Jonnalagadda, Sharma & Agrawal (2023). More recently, the ability of higher-order transport equations to address canonical wall-bounded flows in the slip and transition regimes has been investigated.…”
In this work, we analyse wall-bounded flows in the continuum to transition regime with the help of higher-order transport equations (super-set of the Navier–Stokes equation). Towards this, we incorporate second-order in Knudsen number accurate terms in the single-particle distribution function, and with this complete representation, we first derive the second-order accurate extended-OBurnett (EOBurnett) and third-order accurate super-OBurnett (SOBurnett) equations. We then demonstrate that these newly derived equations exhibit unconditional linear stability. We finally validate the equations by solving for plane Poiseuille flow and derive closed-form analytical solutions for the pressure and velocity fields. The pressure and velocity results thus obtained have been compared with direct simulation Monte Carlo (DSMC) data in the transition regime. The results from both the EOBurnett and SOBurnett equations are found to yield better agreement with DSMC data than that obtained from the Navier–Stokes equations. This improved agreement is attributed to the presence of additional terms in the proposed equations, which effectively capture the effect of the Knudsen layer near the wall. The obtained higher-order transport equations and the closed-form solution presented in this work are novel. The ability of the equations to describe the flow in the transition regime should form the basis for conducting further realistic analytical studies of wall-bounded flows in the future.
“…Similarly, Xu (2003) solved the force-driven plane Poiseuille flow problem by employing the BGK–Burnett and the () BGK–super-Burnett schemes in the Boltzmann equations and demonstrated better results than those obtained using the N-S equations. An alternate way of solving the Boltzmann–BGK equation directly is through the lattice Boltzmann method (LBM) route; recent attempts to employ LBM schemes to solve high- flows have been detailed in Jonnalagadda, Sharma & Agrawal (2023). More recently, the ability of higher-order transport equations to address canonical wall-bounded flows in the slip and transition regimes has been investigated.…”
In this work, we analyse wall-bounded flows in the continuum to transition regime with the help of higher-order transport equations (super-set of the Navier–Stokes equation). Towards this, we incorporate second-order in Knudsen number accurate terms in the single-particle distribution function, and with this complete representation, we first derive the second-order accurate extended-OBurnett (EOBurnett) and third-order accurate super-OBurnett (SOBurnett) equations. We then demonstrate that these newly derived equations exhibit unconditional linear stability. We finally validate the equations by solving for plane Poiseuille flow and derive closed-form analytical solutions for the pressure and velocity fields. The pressure and velocity results thus obtained have been compared with direct simulation Monte Carlo (DSMC) data in the transition regime. The results from both the EOBurnett and SOBurnett equations are found to yield better agreement with DSMC data than that obtained from the Navier–Stokes equations. This improved agreement is attributed to the presence of additional terms in the proposed equations, which effectively capture the effect of the Knudsen layer near the wall. The obtained higher-order transport equations and the closed-form solution presented in this work are novel. The ability of the equations to describe the flow in the transition regime should form the basis for conducting further realistic analytical studies of wall-bounded flows in the future.
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