2018
DOI: 10.1103/physrevx.8.011034
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Branches of Triangulated Origami Near the Unfolded State

Abstract: Origami structures are characterized by a network of folds and vertices joining unbendable plates. For applications to mechanical design and self-folding structures, it is essential to understand the interplay between the set of folds in the unfolded origami and the possible 3D folded configurations. When deforming a structure that has been folded, one can often linearize the geometric constraints, but the degeneracy of the unfolded state makes a linear approach impossible there. We derive a theory for the sec… Show more

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Cited by 38 publications
(66 citation statements)
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“…Self-folding sheets (or self-folding origami) are structures programmed to have one unique low- or zero-energy mode 6 , 29 , 36 . However, self-folding sheets, even when programmed with a single zero-energy mode, have been shown to have exponentially many undesirable misfolding modes accessible from the flat state 14 , 15 . We show how crease stiffness can change the topological connectivity of these modes and leave only the desired folding mode accessible from the flat state.…”
Section: Resultsmentioning
confidence: 99%
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“…Self-folding sheets (or self-folding origami) are structures programmed to have one unique low- or zero-energy mode 6 , 29 , 36 . However, self-folding sheets, even when programmed with a single zero-energy mode, have been shown to have exponentially many undesirable misfolding modes accessible from the flat state 14 , 15 . We show how crease stiffness can change the topological connectivity of these modes and leave only the desired folding mode accessible from the flat state.…”
Section: Resultsmentioning
confidence: 99%
“…When designed, multiple pathways and multistability can be exploited to create mechanical switches, shapeable sheets, and many other metamaterials 2 , 6 12 . However, such nonlinear features can also create problems 10 , 13 15 . For example, self-folding origami, despite the name, has an exponential number of misfolding pathways that meet at a “branch point” at the flat state 13 , 16 – 19 , making it nearly impossible to fold into the desired folding mode 14 , 15 , 20 , 21 .…”
Section: Introductionmentioning
confidence: 99%
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“…Such pursuits typically focus on rigid origami, which concerns perfectly stiff plates connected by flexible hinges that are agnostic as to their mountain-valley (MV) assignment. The absence of a presupposed MV pattern opens up the possibility of pluripotent origami-crease patterns that can fold into multiple 3D target shapes [16][17][18][19] . However, the assumption of rigid plates leads to complex compatibility conditions that make designing foldable patterns notoriously difficult.…”
mentioning
confidence: 99%
“…Once folded, an ideally rigid origami mechanism is constrained to a limited set of trajectories, but when the mechanism is in the flat-unfolded state, it is in a kinematic singularity. From this point, the mechanism can bifurcate into two or more configurations, each with a distinct shape and kinematic behavior, by changing the directions of its folds [referred to collectively as the mountain-valley (MV) assignment] [15]. In physical specimens, the crease pattern is usually fixed during fabrication, but the MV assignment can be changed, presenting a practical approach to transformation.…”
mentioning
confidence: 99%