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This article proposes the concept of anisotropy tailoring in multi-material lattices based on a mechanics-based bottom-up framework. It is widely known that isotropy in a mono-material lattice can be obtained when the microstructure has an isotropic geometry. For example, regular hexagonal lattices with a unit cell comprised of six equal members and equal internal angle of 120^o each, show isotropy in the elastic properties. Such limited microstructural configuration space for having isotropy severely restricts the scope of many multi-functional applications such as space filling in 3D printing. We first demonstrate that there are multiple structural geometries in mono-material lattices that could lead to isotropy. It is shown that the configuration space for isotropy can be expanded by multiple folds when more than one intrinsic material is introduced in the unit cell of a lattice. We explicitly demonstrate different degrees of anisotropy in regular geometrically isotropic lattices by introducing the multi-material architecture. The contours of achieving minimum anisotropy, maximum anisotropy and a fixed value of anisotropy are presented in the design space consisting of geometric and multi-material parameters. Proposition of such multi-material microstructures could essentially expand the multi-functional design scope significantly, offering a higher degree of flexibility to the designer in terms of choosing (or identifying) the most suitable microstructural geometry. An explicit theoretical characterization of the contours of anisotropy along with physical insights underpinning the configuration space of multi-material and geometric parameters will accelerate the process of its potential exploitation in various engineered multi-functional materials and structural systems across different length-scales with the demand of any specific degree of anisotropy but limitation in the micro-structural geometry.
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120o
θ
E1E2E3
E1=E2=E3=Esθ
120o
¯
E1¯
E2
E1E2
θh
l
h/l = 1 θ= 30oα= 1
θh
lα=E1
E2
θ α h
l
h/l = 1 θ= 30oα= 1
α= 1 θh
l
¯
E1= 2Es(t/l)3cos θ
(h/l + sin θ) sin2θ(1 + α)
¯
E2=Es(t/l)3(h/l + sin θ)(1 + α)
2αcos3θ
E1
E2=α E1=αE2=EsE1E2
q=¯
E1
¯
E2
¯
E1¯
E2
E1E2
t
¯
E1¯
E2h l θ
α= 1
¯
E1¯
E2α
α
¯
E1¯
E2
α
α= 1
α
¯
E1¯
E2
α6= 1 h/l θ α
¯
E1=¯
E2h/l = 1 θ= 30oα= 1
α= 1 ¯
E1=¯
E2
4α
(1 + α)2cos4θ
sin2θ= (h/l + sin θ)2
α
α
cos4θ
sin2θ= (h/l + sin θ)2
h/l + sin θ=cos2θ
sin θ
sin θ=1
4
h
l±sh
l2
+ 8
h/l θ
h/l = 1 θ= 30o
h/l = 1 θ= 30oθ=90o
h/l + sin θ=cos2θ
sin θ
sin θ=l
h
h l θ
θ60
h>2lsin θ
¯
E1=¯
E2=Es
sin θcos θt
l3
θ
¯
E1¯
E2
θ= 30oh=l
h/l = 1 θ= 30o
4α
(1 + α)2=1
K
1
K=sin2θ
cos4θh
l+ sin θ2
α=E1
E2
=1+2K±2K+K2
K2K>0
α
q=¯
E1
¯
E2
q=¯
E1
¯
E2=α
(1 + α)2m
m=4 cos4θ
(h/l+sin θ)2sin2θ
qdq
= 0 α
α= 1 d2q
2α=1 <0E1=E2
q= 0.5
q= 1.5q= 2 q= 3
q=¯
E1
¯
E2α=E1
E2θ
h
lθ
(qα
max|α=1) = cos4θ
h
l+ sin θ2
sin2θ
q
h
lθ
E1
E2=α
q¯
E1
¯
E2=q
α
(1 + α)2=q
m
α=E1
E2
=1
2"2q
m±r2q
m24#
E1E2
"2q
m±r2q
m24#>0
2q
m24>0
θ q
α=E1
E2= 1
θ
h/l = 1
θ= 30oα= 1

Supplementary resource (1)

... Honeycomb lattices are extensively used in engineering structures as these provide a structure with minimal density with ecient surface lling, high energy absorption capacity under crushing and impact, high strength to weight ratio, and relatively high out-of-plane compression and shear properties [1,20,21]. In the development of metamaterials by micro-scale architecturing of periodic beam-like networks, heaxagonal lattices and its derivatives (such as square, rhombic and auxetic congurations) have widely been investigated for eective property modulation at the macro scale [22,23,24,25,26]. ...
... Further, since we aim to deal with evaluating the eective linear elastic properties of the lattice here with the assumption of innite (or large) number of unit cells,`size eect' would not have a signicant eect in the current analysis [1,3]. The idea of anisotropy tailoring in lattices with multi-material properties is demonstrated in [22], where the considered unit cell has constituent elements of multiple materials. Active elastic property modulation with the help of voltage has been realized in a recent work [23]. ...
... The overall strain in direction 3 is calculated using equation (22). ...
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Analytical investigations to characterize the effective mechanical properties of lattice materials allow an in-depth exploration of the parameter space efficiently following an insightful, yet elegant framework. 2D lattice materials, which have been extensively dealt with in the literature following analytical as well as numerical and experimental approaches, have limitations concerning multi-directional stiffness and Poisson's ratio tunability. The primary objective of this paper is to develop mechanics-based formulations for a more complex analysis of 3D lattices, leading to a physically insightful analytical approach capable of accounting the beam-level mechanics of pre-existing intrinsic stresses along with their interaction with 3D unit cell architecture. We have investigated the in-plane and out-of-plane effective elastic properties to portray the physics behind the deformation of 3D lattices under externally applied far-field normal and shear stresses. The considered effect of beam-level intrinsic stresses therein can be regarded as a consequence of inevitable temperature variation, pre-stress during fabrication, inelastic and non-uniform deformation, manufacturing irregularities etc. Such effects can notably impact the effective elastic properties of lattice materials, quantifying which for 3D honeycombs is the central focus of this work. Further, from the material innovation viewpoint, the intrinsic stresses can be deliberately introduced to expand the microstructural design space for effective elastic property modulation of 3D lattices. This will lead to programming of effective properties as a function of intrinsic stresses without altering the microstructural geometry and lattice density. We have proposed a generic spectral framework of analyzing 3D lattices analytically, wherein the beam-level stiffness matrix including the effect of bending, axial, shear and twisting deformations along with intrinsic stresses can be coupled with the unit cell mechanics for obtaining the effective elastic properties.
... Very pioneer work for evaluating the effective equivalent elastic properties of regular mono-material conventional honeycomb cells is presented by Gibson et al. [1]. Later, Mukhopadhyay et al. [2] explored the possibilities of anisotropy tailoring of properties through the multi-material arrangement in a symmetric honeycomb lattice. Recently, Sinha et al. [3] proposed a lattice to obtain the elastic modulus and consider the effect of residual stresses. ...
... Then, new parametric results are presented for the in-plane elastic modulus. The literature of Gibson and Ashby [1] and Mukhopadhyay et al. [2] are considered to show excellent agreement with elastic modulus E 1 and E 2 for the present formulation. In Gibson's study, axial, bending, and shear modes of deformations have been considered for an auxetic mono-material case, while in Mukhopadhyay's work [2], a multi-material auxetic structure under only bending deformation is analyzed. ...
... The literature of Gibson and Ashby [1] and Mukhopadhyay et al. [2] are considered to show excellent agreement with elastic modulus E 1 and E 2 for the present formulation. In Gibson's study, axial, bending, and shear modes of deformations have been considered for an auxetic mono-material case, while in Mukhopadhyay's work [2], a multi-material auxetic structure under only bending deformation is analyzed. In Fig. 2, the variation of elastic properties (E 1 and E 2 ) under the influence of axial, bending, and shear effects is plotted for a mono-material auxetic honeycomb structure for different cell angles (θ ). ...
... Generally, a unit cell-based approach is adopted to design lattice metamaterials with a single type of intrinsic material [37] (refer to Figure 1(a, d)). Recently, multi-material lattices have been proposed where dierent cell walls in the unit cells have dierent intrinsic material properties (refer to Figure 1(b)) [60]. With the progress of multi-material additive manufacturing, such lattices can be physically realized with adequate precision [61,62,63,64,65]. ...
... If we further apply the condition for multi-material symmetric hexagonal structure (θ 2 =θ 3 = θ), then we can obtain the expressions for deection of cell wall 2 and 3 under only bending deformation, similar to the case of Mukhopadhyay et al. [60]. ...
... The concept of multi-material hexagonal honeycombs (symmetric structure) and concerned analyses of eective elastic moduli were rst presented by Mukhopadhyay et al. [60]. In that analysis, beam-level deformation was considered based on bending with the assumption of thin cell walls. ...
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... While a wide range of effective material properties can be achieved in such passive material microstructures, the properties cannot be tuned in an on-demand basis after they are manufactured. The recent developments in this direction include bi-level topology architected optimum metamaterials [5], hierarchical metamaterials [24], disordered metamaterials [25], anti-curvature metamaterils with programmed curvature [26,27,28,29], multi-material and space-filled lattices [30,31], origami and kirigami-inspired metamaterials [32,19], to mention a few. Recently the concept of pneumatic elastostatics and deployability in mechanical metamaterials has been proposed based on inflatable lattices that can exhibit extreme specific stiffness along with on-demand tunability [33]. ...
... Now, the slack variables have to be positive to keep the iterations running in the feasible domain. For each of γ > 0, we have Equation 30. ...
... method considering slack variables (refer toEquation 29 and Equation30) to tackle the subproblems that arise throughout the iteration. First, an ideal subproblem is put up in the sequential quadratic programming model to look for the following feasible point in the present iteration point. ...
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... Xu et al. [13] modied the traditional regular honeycomb into AuxHex structure (unit cells with both auxetic and hexagonal honeycomb patterns) in their study and derived the eective elastic moduli and plastic collapse stresses of the lattice. Mukhopadhyay et al. [14] developed the theory for heterogeneous multi-material lattices, while Mukherjee and Adhikari [15] further extended the theory to incorporate beam-level axial and shear deformations. Mukhopadhyay et al. [16] derived the closed-form elastic-moduli expressions of multi-material honeycomb lattices considering the eect of ller material. ...
... For auxetic lattice, the geometrical constraint i.e. L R + 2 sin θ > 0 is conformed so that the vertices of the interior cell member remain untouched during the manufacturing and deformation [14,46]. In the gures, unfeasible geometry indicates the combination of those L R and θ where the aforementioned geometric constraints are being violated. ...
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