Morphological transition in the instability of surface-attached hydrogel films
ORAL
Abstract
Hydrogels may swell drastically when brought in contact with solvent, as driven by gradients of osmotic pressure, resulting in a change in volume that depends on the swelling ratio. For poly-N-isopropylacrylamide gels (PNIPAM), the ratio of wet-to-dry volume is usually a few hundred percent. However, grafting hydrogel films onto a rigid substrate geometrically constrains the swelling. The formation of a surface pattern can result of swelling-induced in-plane stresses.
We study the formation of patterns observed at the surface of PNIPAM-hydrogel films grafted onto silicon wafers, with dry thickness varying from 10 nm to 5 µm. After crosslinking, swelling in a good solvent, combined with subsequent drying in ambient air, gives rise to a plethora of morphologies. Among them, we can see creases and more complex shapes that depend on the wet/dry state of the sample. We observe that both the dry and wet wavelengths of the pattern scale with the initial dry thickness, with a logarithmic correction involving a relevant length scale. The choice of this length scale may involve the pore size or the elasto-capillary length, depending on thickness. The agreement between the resulting correction and the experimental data gives clues for explaining the underlying mechanism of pattern formation.
We study the formation of patterns observed at the surface of PNIPAM-hydrogel films grafted onto silicon wafers, with dry thickness varying from 10 nm to 5 µm. After crosslinking, swelling in a good solvent, combined with subsequent drying in ambient air, gives rise to a plethora of morphologies. Among them, we can see creases and more complex shapes that depend on the wet/dry state of the sample. We observe that both the dry and wet wavelengths of the pattern scale with the initial dry thickness, with a logarithmic correction involving a relevant length scale. The choice of this length scale may involve the pore size or the elasto-capillary length, depending on thickness. The agreement between the resulting correction and the experimental data gives clues for explaining the underlying mechanism of pattern formation.
*This work benifited from the finantial support of ANR with the CoPinS (ANR-19-CE06-0021),EMetBrown (ANR-21-ERCC-0010-01),SOFTER (ANR-21-CE06-0029) and FRICOLAS (ANR-21-CE06-0039) grants and IPGG (Equipex ANR-10-EQPX-34 and Labex ANR-10-LABX-31), EUSMI TA support and expertise of Dr H. Peisker (Nanosurf). We acknowledge financial support from the European Union through the European Research Council under ERC Consolidator grant n°101039103 EMetBrown. Views and opinions expressed are however those of the authors only and do not necessarily reflect those of the European Union or the European Research Council. Neither the European Union nor the granting authority can be held responsible for them.
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Presenters
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Caroline Kopecz-Muller
- ESPCI Paris