2018
DOI: 10.1016/j.camwa.2018.04.008
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A framework for FFT-based homogenization on anisotropic lattices

Abstract: In order to take structural anisotropies of a given composite and different shapes of its unit cell into account, we generalize the Basic Scheme in homogenization by Moulinec and Suquet to arbitrary sampling lattices and tilings of the d-dimensional Euclidean space. We employ a Fourier transform for these lattices by introducing the corresponding set of sample points, the so called pattern, and its frequency set, the generating set, both representing the anisotropy of both the shape of the unit cell and the ch… Show more

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Cited by 4 publications
(12 citation statements)
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“…With these definitions the discretisation of the PDEs on spaces of translates can be performed as follows: Choosing the function f as the Dirichlet kernel f = D M reduces (18) and (20) to discretised equations which correspond to truncating the Fourier series arising in the continuous equations (11) and (12). The effect of the pattern matrix M in this special case is analysed in [2]. For the Dirichlet kernel on a tensor product grid, which corresponds to a diagonal pattern matrix, Vondřejc et.al.…”
Section: Approximation Of Periodic Pde Solutionsmentioning
confidence: 99%
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“…With these definitions the discretisation of the PDEs on spaces of translates can be performed as follows: Choosing the function f as the Dirichlet kernel f = D M reduces (18) and (20) to discretised equations which correspond to truncating the Fourier series arising in the continuous equations (11) and (12). The effect of the pattern matrix M in this special case is analysed in [2]. For the Dirichlet kernel on a tensor product grid, which corresponds to a diagonal pattern matrix, Vondřejc et.al.…”
Section: Approximation Of Periodic Pde Solutionsmentioning
confidence: 99%
“…The generalized Hashin structure that consists of two confocal ellipsoids (Ω c ) and (Ω e ) embedded in a matrix material (Ω m ) and is depicted in Figure 2 (left). For this structure an analytic expression for the strain ε and for the effective stiffness C eff : ε 0 is known and described in [2,Section 4.2]. The examples were computed using (18) using an iterative scheme based on a Neumann series approach, originally proposed by Moulinec and Suquet [9].…”
Section: Numerical Examplesmentioning
confidence: 99%
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“…[27] show that the method of Moulinec and Suquet can also be understood as a Galerkin projection using truncated Fourier series. This idea is generalized in [3] to anisotropic lattices thus allowing to take directional information on the geometrical structure or the orientation of interfaces between materials into account. Brisard and Dormieux [8,9] use constant finite elements to arrive at the Basic Scheme with a modified linear operator, based on an energy based formulation.…”
Section: Introductionmentioning
confidence: 99%