Snapping and switching of elastic arches with patterned preferred curvature

An elastic arch is an archetypal bistable system. Here, we combine elastica theory and photo-mechanical experiments to elucidate the mechanics of an active arch with a spatio-temporally varying preferred curvature κ(s). Our shallow-arch theory completely describes any such system via the decomposition of its κ(s) into Euler-buckling modes. Intuitively, if κ(s) overlaps with the fundamental mode, it snaps the arch up/down. Conversely, non-overlapping κ(s) drives a second-order transition to a higher-order shape. Furthermore, the form of κ(s) enables control over the instability’s character; we find the forms for snapping with maximum energy release and at the lowest stimulation (both binary patterns) and design forms for symmetric and asymmetric switching pathways. Analogous control can also be achieved in boundary-driven instabilities of passive arches by fabricating them with suitable κ(s). We thus anticipate our results will improve switchable/snapping elements in MEMS, robotics, and mechanical meta-materials.

Authors

Publication Details

Journal
Apollo
Published
2026-07-02
DOI
https://doi.org/10.17863/cam.131848
Primary Topic
Advanced Materials and Mechanics
Type
article
Field-Weighted Citation Impact
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article

Snapping and switching of elastic arches with patterned preferred curvature

John Biggins, Ammar Khan, Michal Zmyslony
Apollo
Advanced Materials and Mechanics
article

Snapping and switching of elastic arches with patterned preferred curvature

John Biggins, Ammar Khan, Michal Zmyslony
article en

Abstract

An elastic arch is an archetypal bistable system. Here, we combine elastica theory and photo-mechanical experiments to elucidate the mechanics of an active arch with a spatio-temporally varying preferred curvature κ(s). Our shallow-arch theory completely describes any such system via the decomposition of its κ(s) into Euler-buckling modes. Intuitively, if κ(s) overlaps with the fundamental mode, it snaps the arch up/down. Conversely, non-overlapping κ(s) drives a second-order transition to a higher-order shape. Furthermore, the form of κ(s) enables control over the instability’s character; we find the forms for snapping with maximum energy release and at the lowest stimulation (both binary patterns) and design forms for symmetric and asymmetric switching pathways. Analogous control can also be achieved in boundary-driven instabilities of passive arches by fabricating them with suitable κ(s). We thus anticipate our results will improve switchable/snapping elements in MEMS, robotics, and mechanical meta-materials.

Apollo
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Advanced Materials and Mechanics
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