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arXiv 2602.16486physics.flu-dynphysics.comp-ph
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基于正交中心矩的波动格子Boltzmann方法

A fluctuating lattice Boltzmann formulation based on orthogonal central moments

The University of Manchester(曼彻斯特大学)

Alessandro De Rosis, Yang Zhou

AI总结:

本文提出一种基于正交中心矩的波动格子Boltzmann方法,通过引入随机强迫和模式依赖弛缓,实现精确满足波动-耗散定理,验证了热化、各向同性和速度波动标度关系。

摘要:

热波动在介观尺度的流体动力学中起着核心作用,必须以符合统计力学的方式纳入数值方案中。在本工作中,我们开发了一种基于正交中心矩表示的波动格子Boltzmann方法。在中心矩的空间中直接引入随机强迫,并与模式依赖的弛缓一致配对,从而得到一个满足波动-耗散定理的离散动力学模型。由于基函数的正交性,中心矩的平衡协方差矩阵是对角的,每个非守恒模式可以被解释为一个独立的离散奥本海姆-乌尔申贝克过程,其方差由平衡热力学固定。所得到的模型在平衡时保证动能的精确均分,保持伽利略不变性,并保留了基于中心矩的碰撞算子的增强数值稳定性特征。为D2Q9和D3Q27晶格构造了显式波动方案。还讨论了向降速离散化的扩展。一组全面的数值测试验证了热化、平衡统计的各向同性以及速度波动与热能、密度和弛缓时间的预期标度关系。与波动BGK方法相比,本方法在过弛缓区域保持稳定和良好设定,包括在稳定性极限附近。这些结果表明,基于中心矩的格子Boltzmann方法为波动流体动力学提供了一个自然且稳健的框架,在离散层面,耗散、噪声和动能模式结构得以一致地对齐。

英文摘要:

Thermal fluctuations play a central role in fluid dynamics at mesoscopic scales and must be incorporated into numerical schemes in a manner consistent with statistical mechanics. In this work, we develop a fluctuating lattice Boltzmann formulation based on an orthogonal central-moments-based representation. Stochastic forcing is introduced directly in the space of central moments (CMs) and consistently paired with mode-dependent relaxation, yielding a discrete kinetic model that satisfies the fluctuation-dissipation theorem exactly at the lattice level. Owing to the orthogonality of the basis, the equilibrium covariance matrix of the central moments is diagonal, and each non-conserved mode can be interpreted as an independent discrete Ornstein-Uhlenbeck process with variance fixed by equilibrium thermodynamics. The resulting formulation guarantees exact equipartition of kinetic energy at equilibrium, preserves Galilean invariance, and retains the enhanced numerical stability characteristic of CMs-based collision operators. Explicit fluctuating schemes are constructed for the D2Q9 and D3Q27 lattices. The extension to reduced-velocity discretisation is discussed too. A comprehensive set of numerical tests verifies correct thermalisation, isotropy of equilibrium statistics, and the expected scaling of velocity fluctuations with thermal energy, density, and relaxation time. In contrast to fluctuating BGK formulations, the present method remains stable and well posed in the over-relaxation regime, including in the immediate vicinity of the stability limit. These results demonstrate that CMs-based lattice Boltzmann methods provide a natural and robust framework for fluctuating hydrodynamics, in which dissipation, noise, and kinetic mode structure are consistently aligned at the discrete level.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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