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Deriving hydrodynamic equations for lattice systems

机译:推导晶格系统的流体动力学方程

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We study the dynamics of lattice systems in ? ~d, d ≥ 1. We assume that the initial data are random functions. We introduce the family of initial measures {μ 0 ~(e{open}), e{open} > 0}. The measures μ 0 ~(e{open}) are assumed to be locally homogeneous or "slowly changing" under spatial shifts of the order o(e{open} ~(-1)) and inhomogeneous under shifts of the order e{open} ~(-1). Moreover, correlations of the measures μ 0 ~(e{open}) decrease uniformly in e{open} at large distances. For all τ ∈ ? 0, r ∈ ? ~d, and κ > 0, we consider distributions of a random solution at the instants t = τ/e{open} κ at points close to [r/e{open}] ∈ ? ~d. Our main goal is to study the asymptotic behavior of these distributions as e{open} → 0 and to derive the limit hydrodynamic equations of the Euler and Navier-Stokes type.
机译:我们研究了?中的晶格系统动力学。 〜d,d≥1。我们假设初始数据为随机函数。我们介绍了一系列初始量度{μ0〜(e {open}),e {open}> 0}。假设量度μ0〜(e {open})在阶数o(e {open}〜(-1))的空间位移下是局部均匀的或“缓慢变化的”,而在阶数e {open的位移下是非均匀的}〜(-1)。此外,在远距离处,度量e 0〜(e {open})的相关性在e {open}中均匀减小。对于所有τ∈? 0,r∈? 〜d,且κ> 0时,我们考虑在t =τ/ e {open}κ时刻[r / e {open}]∈?附近的随机解的分布。 〜d。我们的主要目标是研究当e {open}→0时这些分布的渐近行为,并推导Euler和Navier-Stokes类型的极限流体动力学方程。

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