Abstract

Radial basis function generated finite differences (RBF-FD) represent the latest discretization approach for solving partial differential equations. Their benefits include high geometric flexibility, simple implementation, and opportunity for large-scale parallel computing. Compared to other meshfree methods, typically based upon moving least squares (MLS), the RBF-FD method is able to recover a high order of algebraic accuracy while remaining better conditioned. These features make RBF-FD a promising candidate for kinetic-based fluid simulations such as lattice Boltzmann methods (LB). Pursuant to this approach, we propose a characteristic-based off-lattice Boltzmann method (OLBM) using the strong form of the discrete Boltzmann equation and radial basis function generated finite differences (RBF-FD) for the approximation of spatial derivatives. Decoupling the discretizations of momentum and space enables the use of irregular point cloud, local refinement, and various symmetric velocity sets with higher order isotropy. The accuracy and computational efficiency of the proposed method are studied using the test cases of Taylor–Green vortex flow, lid-driven cavity, and periodic flow over a square array of cylinders. For scattered grids, we find the polyharmonic spline + poly RBF-FD method provides better accuracy compared to MLS. For Cartesian node layouts, the results are the opposite, with MLS offering better accuracy. Altogether, our results suggest that the RBF-FD paradigm can be applied successfully also for kinetic-based fluid simulation with lattice Boltzmann methods.

Highlights

  • The coupling between momentum space and physical space restricts the method to uniform Cartesian grids, which are often disadvantageous for the study of flow in complex geometries [12]

  • Given the shortcoming of the weak-form meshfree lattice Boltzmann method (LBM), it is natural to wonder whether or not their strong-form cousins are more suitable candidates for computational kinetic simulations with discrete velocity models such as LBM. We demonstrate this notion by developing a strong-form off-lattice Boltzmann method (OLBM) (SFOLBM) for irregular point clouds

  • We have introduced a strong-form off-lattice Boltzmann method (SFOLBM) based upon the Lax–Wendroff discretization in time and an Radial basis function generated finite differences (RBF-FD) or moving least squares (MLS)

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Summary

Introduction

The main properties underlying this success include the algorithmic simplicity of the method with its particle-like nature, a high parallel efficiency due to the large degree of local operations, and the simple handling of boundary conditions via bounce-back type methods [10,11], among others These properties are a result of the ingenious coupling between the velocity and spatial discretizations in such a way that the spatial grid corresponds to the characteristics of the discrete velocity space [12]. The standard lattice symmetric stencils in 2-d and 3-d, that is, those including only the neighbors from the first Brillouin zone, such as D2Q9 and D3Q19, do not guarantee sufficient degrees of freedom and lead to the loss of Galilean invariance at finite Mach numbers This limits LBM’s domain of applicability to weakly-compressible athermal flows [14,15]. While several existing integer-based multi-speed lattices can overcome this issue and simultaneously extend

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