2022
DOI: 10.1016/j.matdes.2022.110532
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A non-centrosymmetric square lattice with an axial–bending coupling

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Cited by 9 publications
(5 citation statements)
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“…The outputs of this latch depend not only on the current input but also on the operation being performed, such as holding previous values or setting new ones. A mechanical SR latch can be physically implemented by breaking the centrosymmetry in an assembly of two mechanical transistors [ 49 ] to create a local closed loop that circulates heat, providing Q now and Q next outputs, as illustrated in Figure 3b. Periodic set‐reset experiments confirmed the SR latch's functionality, shown in Figure 3c.…”
Section: Resultsmentioning
confidence: 99%
“…The outputs of this latch depend not only on the current input but also on the operation being performed, such as holding previous values or setting new ones. A mechanical SR latch can be physically implemented by breaking the centrosymmetry in an assembly of two mechanical transistors [ 49 ] to create a local closed loop that circulates heat, providing Q now and Q next outputs, as illustrated in Figure 3b. Periodic set‐reset experiments confirmed the SR latch's functionality, shown in Figure 3c.…”
Section: Resultsmentioning
confidence: 99%
“…To conclude, our combined semi‐analytical, experimental, and numerical investigations have shown that symmetry breaking of slit pattern induces geometric frustration and anisotropic shape morphing in bistable kirigami and controls the trade‐offs between bistability and anisotropy of scaling. While symmetry breaking has been used to generate anisotropic response in other metamaterial architectures, [ 29,41,44,52 ] this work unlocks anisotropic morphing in kirigami metamaterials and further unveils how symmetry groups affect geometric frustration and their anisotropic bistable shape shifting. For example, “p31m” BAM with threefold rotational symmetry features frustration‐free bistable isotropic expansion, “cm” ABAM with lower symmetry undergoes frustrated anisotropic deployment with reduced bistability, and “p1” ABAM with least symmetry exhibits a moderate response that is frustrated and bounded by “cm” ABAM.…”
Section: Discussionmentioning
confidence: 99%
“…[41] Symmetry has long been a valuable tool for creating complex architected materials. [41][42][43][44] However, for kirigami metamaterials it has only been applied to rigid deployable patterns [28,29,45] with kinematics described by nondeformable panels and pure rotational hinges. The deployment of all these patterns does not involve geometric frustration, [46,47] a phenomenon occurring when incompatible geometric constraints impede the deformation of an object under a set of applied forces; in the realm of kirigami, geometric frustration appears as local disordered deployments caused by incompatible geometric restrictions, such as local deformation of panels due to slit geometry that violates rigid deployable constraints [48] and out-of-plane morphing due to nonuniform strains in nonperiodic patterns.…”
Section: Introductionmentioning
confidence: 99%
“…Mechanical coupling can provide an interactive design that can communicate with adjacent units. [23] Beyond the most wellknown mechanical coupling (Poisson's effect), lattice structures can produce anisotropic mechanical couplings such as axial-shear, [20] axial-bending, [24] and axial-twist couplings [25] by breaking the symmetry of regular lattices. [26] Figure 4 and Video S4 (Supporting Information) show multimodal mechanical couplings of 2D lattices by reprogramming with structural instability and asymmetric magnetization.…”
Section: Multimodal Mechanical Couplings By Reprogrammable Transforma...mentioning
confidence: 99%