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Buckling and unraveling Poly(N-isopropyl acrylamide)-Thermoplastic Polyurethane bilayers

Title data

Agarwal, Seema ; Yarin, Alexander L.:
Buckling and unraveling Poly(N-isopropyl acrylamide)-Thermoplastic Polyurethane bilayers.
In: Polymer. Vol. 97 (2016) Issue 5 . - pp. 604-613.
ISSN 0032-3861
DOI: https://doi.org/10.1016/j.polymer.2016.05.057

Abstract in another language

The theory of two-dimensional Poly(N-isopropyl acrylamide)-Thermoplastic Polyurethane (PNIPAM-TPU) bilayers and of three-dimensional PNIPAM-TPU bilayer filaments is developed. This is the first theory which provides a comprehensive explanation and a detailed description of buckling of PNIPAM-TPU bilayers, as to our knowledge. In agreement with the experimental evidence it reveals that being immersed in a water bath at temperature T < LCST (the lower critical solution temperature), water infiltration into the porous PNIPAM layer of the bilayer begins resulting in swelling and stretching. Being inevitably perturbed (not perfectly straight) at the beginning, a long thin bilayer begins to buckle. However, its buckling is not identical to that of the elastic Euler bars, since the PNIPAM layer in the bilayer is loaded by a distributed compressive force imposed by the bonded TPU layer, while the Euler bars are loaded by compressive forces only at the ends. It is shown that when buckling bilayer stays in the cold bath at T < LCST for a long enough time, its stretching practically stops. However, its buckling continues for a while, since the longitudinal compressive force acting on the PNIPAM layer from the bonded TPU layer permanently exists. That results in self-coiling of the bilayer, which continues until a steady-state coiled configuration is achieved. It is shown that the steady-state coil radius is of the order of the bilayer thickness, much less than the original bilayer length, because the bilayer buckling is driven by a longitudinally distributed compressive force rather than by the compressive force applied only at the ends (like in the classical Euler buckling when the final radius of curvature is of the order of the bar length). If alternatively, after some period of swelling, stretching and buckling, water in the bath is replaced by hot water at T > LCST, water outflow from the PNIPAM-TPU bilayer begins and it shrinks to its original short length and a practically straight initial configuration. When a PNIPAM-TPU bilayer is immersed directly in a water bath at T > LCST, the PNIPAM layer begins to shrink, thus compressing the TPU layer, which in turn, triggers buckling. Long PNIPAM-TPU bilayer filaments, being submerged in water bath at T < LCST, buckle as a circular helix with its radius of curvature and pitch decreasing in time.

Further data

Item Type: Article in a journal
Refereed: Yes
Institutions of the University: Faculties > Faculty of Biology, Chemistry and Earth Sciences
Faculties > Faculty of Biology, Chemistry and Earth Sciences > Department of Chemistry
Faculties > Faculty of Biology, Chemistry and Earth Sciences > Department of Chemistry > Chair Macromolecular Chemistry II
Result of work at the UBT: Yes
DDC Subjects: 500 Science > 540 Chemistry
Date Deposited: 14 Aug 2018 09:33
Last Modified: 14 Aug 2018 09:33
URI: https://eref.uni-bayreuth.de/id/eprint/45426