2017
DOI: 10.1039/c7sm01013c
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Transition of surface–interface creasing in bilayer hydrogels

Abstract: Controlling the morphologies and properties of the surface and/or interface of bimaterials consisting of soft polymers provides new opportunities in many engineering applications. Crease is a widely observed deformation mode in nature and engineering applications for soft polymers where the smooth surface folds into a region of self-contact with a sharp tip, usually induced by the instability from mechanical compression or swelling. In this work, we explore the competition mechanisms between surface and interf… Show more

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Cited by 16 publications
(10 citation statements)
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“…global harmonic waves) and/or creasing (i.e. localized sharp folds) [10,11,12,13,14,15,16,17,18,19,20], as illustrated in Figure 1. While creasing mainly occurs as the first mode of instability when homogeneous gels are exposed to large swelling [12,18], wrinkling patterns are first and foremost found in gels having a gradient stiffness through the thickness, caused by a variation in the crosslinking density within the gel [14,21,22], or by the deposition of a thin and stiff film at the outer surface of the gel, possibly to alter properties like permeability, stability or biocompatibility [23,24,25].…”
Section: Introductionmentioning
confidence: 99%
“…global harmonic waves) and/or creasing (i.e. localized sharp folds) [10,11,12,13,14,15,16,17,18,19,20], as illustrated in Figure 1. While creasing mainly occurs as the first mode of instability when homogeneous gels are exposed to large swelling [12,18], wrinkling patterns are first and foremost found in gels having a gradient stiffness through the thickness, caused by a variation in the crosslinking density within the gel [14,21,22], or by the deposition of a thin and stiff film at the outer surface of the gel, possibly to alter properties like permeability, stability or biocompatibility [23,24,25].…”
Section: Introductionmentioning
confidence: 99%
“…The initial chemical potential μ0 is negative in the formula. Readers are referred to our recent work for more details [51]. The first Piola–Kirchhoff (PK) stress can be derived as Pij=WFij=KTυNvϕ01/3Fij+[]1Nvϕ0Jμ0+μKT+χϕ02J2+lnJϕ0JJF1ji.…”
Section: Numerical Analysismentioning
confidence: 99%
“…( a ) The mechanical test machine and the cylindrical specimen through which we obtained the force–strain curves for hydrogels (reproduced from Ref. [51] with permission from The Royal Society of Chemistry.) ( b ) The finite element (FE) mesh used to calibrate the material parameters of the hydrogel.…”
Section: Figurementioning
confidence: 99%
“…Additionally, in an effort to improve mechanical properties and stability of bilayer hydrogels in environments with different pH, this study also compared PAA-PVA thin films made by conventional techniques to PAA-PVA bilayers fabricated as IDNs. Delamination, 29,30 the impact of IDN hydrogels in actuation of the bilayers, and their corresponding drug release profile are characterized. Additionally, since bending deflections have previously been reported by measuring bending angle 31 or displacement distance from the zero order, 32 the bending strain of the developed bilayers are measured directly using a strain gauge in order to better quantify bilayer efficacy under stimulus.…”
Section: Introductionmentioning
confidence: 99%