Effect of imperfect interface on the effective properties of elastic micropolar multilaminated nanostructures

Author:

Espinosa‐Almeyda Yoanh1ORCID,Yanes Victor2ORCID,Rodríguez‐Ramos Reinaldo3ORCID,Otero José A.4ORCID,Sánchez‐Valdés César F.1ORCID,Camacho‐Montes Héctor1ORCID,Longoria Pablo Padilla5ORCID,Sabina Federico J.5ORCID

Affiliation:

1. Instituto de Ingeniería y Tecnología Universidad Autónoma de Ciudad Juárez Chihuahua México

2. Escuela Técnica Superior de Ingeniería Aeronáutica y del Espacio Universidad Politécnica de Madrid Madrid España

3. Facultad de Matemática y Computación Universidad de La Habana La Habana Cuba

4. Escuela de Ingeniería y Ciencia Tecnológico de Monterrey Estado de México México

5. Instituto de Investigaciones en Matemáticas Aplicadas y en Sistemas Universidad Nacional Autónoma de México CDMX México

Abstract

AbstractIn this paper, the problem of a heterogeneous elastic micropolar nanostructure with a periodic structure subject to imperfect contact conditions is analyzed through the two‐scale asymptotic homogenization method (AHM). The imperfect interface is modeled as a generalization of the well‐known spring model; that is, the homogeneous imperfect interface is described by the following conditions: tractions and coupled stress are continuous, but displacements and microrotations are discontinuous across the imperfect interface. The jumps in displacements and microrotations are proportional to the interface traction and coupled stress components, respectively. In particular, micropolar multilaminated nanocomposites with centro‐symmetric isotropic constituents and imperfect contact conditions are studied. From AHM, the solutions for the displacement and microrotation fields are found by means of two‐scale series expansions depending on a local (microscopic) variable and a global (macroscopic) variable. The local problem statements and the corresponding effective properties are explicitly described. The formulation depends on the constituent physical properties, the imperfection parameters, the cell length in the y3‐direction, and the phase's volume fractions. Numerical results are illustrated and discussed. We concluded that the effective moduli are affected by the imperfections and the cell length in the y3‐direction.

Publisher

Wiley

Subject

Applied Mathematics,Computational Mechanics

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