Implicit-explicit finite-difference lattice Boltzmann method with viscid compressible model for gas oscillating patterns in a resonator
Implicit-explicit finite-difference lattice Boltzmann method with viscid compressible model for gas oscillating patterns in a resonator
ifficulties for the conventional computational fluid dynamics and standard lattice Boltzmann method to study the gas oscillating patterns in a resonator are discussed. In light of the recent progresses in the lattice Boltzmann method world, we are now able to deal with the compressibility and non-linear shock wave effects in the resonator. The implicit-explicit finite-difference lattice Boltzmann method is used to investigate such problem. In particular, a lattice Boltzmann model for viscid compressible flows is introduced firstly. Then, the Boltzmann equation with Bhatnagar-Gross-Krook approximation is solved by a finite-difference method with the third-order implicit-explicit Runge-Kutta scheme for time discretization, and the fifth-order WENO scheme for space discretization. Numerical results obtained in this study agree quantitatively well with available experimental data and simulation results using conventional numerical methods. Moreover, with the implicit-explicit finite-difference lattice Boltzmann method, the computational convergence rate can be significantly improved compared with the previous finite-difference and standard lattice Boltzmann method. This work is carried out as the first effort to study phenomena in thermoacoustics engines with lattice Boltzmann method.
ifficulties for the conventional computational fluid dynamics and standard lattice Boltzmann method to study the gas oscillating patterns in a resonator are discussed. In light of the recent progresses in the lattice Boltzmann method world, we are now able to deal with the compressibility and non-linear shock wave effects in the resonator. The implicit-explicit finite-difference lattice Boltzmann method is used to investigate such problem. In particular, a lattice Boltzmann model for viscid compressible flows is introduced firstly. Then, the Boltzmann equation with Bhatnagar-Gross-Krook approximation is solved by a finite-difference method with the third-order implicit-explicit Runge-Kutta scheme for time discretization, and the fifth-order WENO scheme for space discretization. Numerical results obtained in this study agree quantitatively well with available experimental data and simulation results using conventional numerical methods. Moreover, with the implicit-explicit finite-difference lattice Boltzmann method, the computational convergence rate can be significantly improved compared with the previous finite-difference and standard lattice Boltzmann method. This work is carried out as the first effort to study phenomena in thermoacoustics engines with lattice Boltzmann method.
何雅玲、黄竞、王勇、李庆
热力工程、热机数学力学
Lattice Boltzmann methodimplicit-explicitfinite-differencecompressible flowgas oscillating
Lattice Boltzmann methodimplicit-explicitfinite-differencecompressible flowgas oscillating
何雅玲,黄竞,王勇,李庆.Implicit-explicit finite-difference lattice Boltzmann method with viscid compressible model for gas oscillating patterns in a resonator[EB/OL].(2007-12-25)[2025-08-11].http://www.paper.edu.cn/releasepaper/content/200712-684.点此复制
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