The responsive mechanism of the Venus flytrap has captured the interest of scientists for centuries. Although a complete understanding of the mechanism controlling the Venus flytrap movement has yet to be determined, a recent publication by Forterre et al. [1] demonstrates the importance of geometry and material properties for this fast, stimuliresponsive movement. Specifically, the movement is attributed to a snapthrough elastic instability whose sensitivity is dictated by the length scale, geometry, and materials properties of the features.[2] Here, we use lessons from the Venus flytrap to design surfaces that dynamically modify their topography. We present a simple, robust, biomimetic responsive surface based on an array of microlens shells that snap from one curvature (e.g., concave) to another curvature (e.g., convex) ( Fig. 1) when a critical stress develops in the shell structure. This snap-transition is due to the onset of an elastic, snap-through instability similar to the capture mechanism of the Venus flytrap. The response rates can be over two orders of magnitude faster than the typical response of shape-memory polymers, and the sensitivity and rate of the response can be tuned with predictable geometric and/or material property changes. Based on materials choice, a wide variety of external stimuli can trigger this stress development, such as temperature, pH, solvent swelling, magnetism, electric current, and light. This strategy has great potential for the design of responsive surfaces, which will impact a variety of applications including: release-on-command coatings [3] and adhesives, [4][5][6][7] on-command frictional changes, [8,9] instant modification of optical properties at an interface, [10,11] rapid response drug delivery, [12][13][14] chemical sensing, [15][16][17] and antimicrobial devices. [18] To fabricate the active surface structures, we use the Euler buckling of plates to generate a controlled array of microlens shells under equibiaxial compressive stress (Fig. 2a). First, we pattern cylindrical posts of photoresist onto a silicon wafer and micromold poly(dimethyl siloxane) (PDMS) (Sylgard 184 TM ) elastomer onto it, creating an array of holes. This elastic, PDMS array of holes is then placed in equi-biaxial strain through a simple inflation procedure. A thin film of crosslinked PDMS (typically 15-60 lm in thickness) coated with a thin (∼ 1 lm) layer of uncured PDMS is placed on the surface of the strained holes. The assembly is heated to crosslink the uncured PDMS and bond the film to the array of holes while under equibiaxial tension. Releasing the tension causes an equibiaxial compressive strain to develop in the thin PDMS coating. The associated compressive stresses cause the circular plate of PDMS on the surface of each hole to buckle, thus creating an array of convex microlenses. This technique for microlens preparation is simple, robust, and should be scalable to much smaller length scales across a multitude of materials.
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