This article answers the question of whether homogenization of discrete fine-scale mechanical models, such as particle or lattice models, gives rise to an equivalent continuum that is of Cauchy-type or Cosserat-type. The study employs the machinery of asymptotic expansion homogenization to analyze discrete mechanical models with rotational degrees of freedom commonly used to simulate the mechanical behavior of heterogeneous solids. The proposed derivation has general validity in both stationary (steady-state) and transient conditions (assuming wavelength much larger that particle size) and for arbitrary nonlinear, inelastic fine-scale constitutive equations. The results show that the unit cell problem is always stationary, and the only inertia term appears in the linear momentum balance equation at the coarse scale. Depending on the magnitude of the local bending stiffness, mathematical homogenization rigorously identifies two limiting conditions that correspond to the Cauchy continuum and the Cosserat continuum. A heuristic combination of these two limiting conditions provides very accurate results also in the transition from one limiting case to the other. Finally, the study demonstrates that cases for which the Cosserat character of the homogenized response is significant are associated with non-physically high fine-scale bending stiffness and, as such, are of no interest in practice.
翻译:本文探讨了离散细观力学模型(如粒子模型或晶格模型)的均匀化是否会产生Cauchy型或Cosserat型等效连续体的问题。研究采用渐近展开均匀化方法,分析了常用于模拟非均匀固体力学行为的、具有旋转自由度的离散力学模型。所提出的推导在稳态和瞬态条件下(假设波长远大于粒子尺寸)均具有普适性,且适用于任意非线性、非弹性的细观本构方程。结果表明,单胞问题始终是稳态的,唯一的惯性项出现在粗尺度线性动量平衡方程中。根据局部弯曲刚度的大小,数学均匀化严格识别出两种极限条件,分别对应Cauchy连续体和Cosserat连续体。通过启发式地结合这两种极限条件,在从一个极限情况过渡到另一个极限情况时也能获得非常精确的结果。最后,研究表明,当均匀化响应的Cosserat特性显著时,通常与细观尺度上非物理的高弯曲刚度相关,因此在实践中并无实际意义。