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Effect of solvent hydrophobicity on gelation kinetics and phase diagram of gelatin ionogelsElectronic supplementary information (ESI) available: The data for cg profiles, storage modulus profiles of [C4mim][Cl] and [C6mim][Cl] based ionogels, time dependent viscosity growth and hydrodynamic radii growth profiles of different ionogels and 3D phase diagrams of [C6mim][Cl] based ionogels. See DOI: 10.1039/c3sm52701h

We present a systematic investigation of the effect of solvent hydrophobicity (alkyl chain length) on the gelation kinetics and the phase states of the polypeptide gelatin in imidazolium based ionic liquid (IL) solutions. We have observed that IL concentration and hydrophobicity had dramatic influen...

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Main Authors: Rawat, Kamla, Pathak, Jyotsana, Bohidar, H. B
Format: Article
Language:English
Online Access:Get full text
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Summary:We present a systematic investigation of the effect of solvent hydrophobicity (alkyl chain length) on the gelation kinetics and the phase states of the polypeptide gelatin in imidazolium based ionic liquid (IL) solutions. We have observed that IL concentration and hydrophobicity had dramatic influences on the thermal and viscoelastic properties of gelatin ionogels. Gelation concentration c g was observed to increase from 1.75 to 2.75% (w/v) while the gelation temperature T g was found to decrease from 32 to 26 °C with increase in 1-octyl-3-methyl imidazolium chloride [C8mim][Cl] (most hydrophobic) concentration as compared to the case of the least hydrophobic IL 1-ethyl-3-methyl imidazolium chloride [C2mim][Cl], where the corresponding changes were marginal. Gradual softening of the gel with increase in hydrophobicity and concentration of IL was clearly noticed. The viscosity of the gelling sol diverged as η r ∼ − k 1 and storage modulus of gel grew as G 0 ∼ t 1 where 1 = |1 − c / c g | with the exponents having values k = 1.2-1.8 ± 0.08 and t = 1.2-1.6 ± 0.08, close to but not exactly the same as predicted by the percolation model: k = 0.7-1.3 and t = 1.9. Thus, the gelation kinetics involved in the growth of interconnected networks could be conceived to follow an anomalous percolation model. The temporal growth of self-assembled structures followed a power law dependence given by: η r ∼ − α 2 and R h ∼ − β 2 where , t > t g ( α = 1-2.9 ± 0.08 and β = 1-2.7 ± 0.08). The low frequency storage modulus G 0 , gelation temperature T g , gelation concentration c g and gelation time t g adequately defined the sol-gel phase diagram. Results clearly revealed that by adjusting the hydrophobic chain length and concentration of IL it was possible to customize both thermal and mechanical properties of these ionogels to match specific application requirements. Schematic diagram of gelatin ionogel where the core of the gel is filled with IL aggregates leaving little scope for H-bonds to exist. These voids weaken the network structure.
ISSN:1744-683X
1744-6848
DOI:10.1039/c3sm52701h