Solvation Dynamics in Different Phases of the Lyotropic Liquid Crystalline System

dc.contributor.authorROY, BIBHISANen_US
dc.contributor.authorSatpathi, Sagaren_US
dc.contributor.authorGAVVALA, KRISHNAen_US
dc.contributor.authorKoninti, Raj Kumaren_US
dc.contributor.authorHAZRA, PARTHAen_US
dc.contributor.departmentDept. of Chemistryen_US
dc.date.accessioned2019-03-15T11:22:37Z
dc.date.available2019-03-15T11:22:37Z
dc.date.issued2015-09en_US
dc.description.abstractReverse hexagonal (HII) liquid crystalline material based on glycerol monooleate (GMO) is considered as a potential carrier for drugs and other important biomolecules due to its thermotropic phase change and excellent morphology. In this work, the dynamics of encapsulated water, which plays important role in stabilization and formation of reverse hexagonal mesophase, has been investigated by time dependent Stokes shift method using Coumarin-343 as a solvation probe. The formation of the reverse hexagonal mesophase (HII) and transformation to the L2 phase have been monitored using small-angle X-ray scattering and polarized light microscopy experiments. REES studies suggest the existence of different polar regions in both HII and L2 systems. The solvation dynamics study inside the reverse hexagonal (HII) phase reveals the existence of two different types of water molecules exhibiting dynamics on a 120–900 ps time scale. The estimated diffusion coefficients of both types of water molecules obtained from the observed dynamics are in good agreement with the measured diffusion coefficient collected from the NMR study. The calculated activation energy is found to be 2.05 kcal/mol, which is associated with coupled rotational-translational water relaxation dynamics upon the transition from “bound” to “quasi-free” state. The observed ∼2 ns faster dynamics of the L2 phase compared to the HII phase may be associated with both the phase transformation as well as thermotropic effect on the relaxation process. Microviscosities calculated from time-resolved anisotropy studies infer that the interface is almost ∼22 times higher viscous than the central part of the cylinder. Overall, our results reveal the unique dynamical features of water inside the cylinder of reverse hexagonal and inverse micellar phases.en_US
dc.identifier.citationJournal of Physical Chemistry B, 119 (35), 11721-11731.en_US
dc.identifier.issn1520-6106en_US
dc.identifier.issn1520-5207en_US
dc.identifier.sourcetitleJournal of Physical Chemistry Ben_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/2150
dc.identifier.urihttps://doi.org/10.1021/acs.jpcb.5b04370
dc.language.isoenen_US
dc.publication.originofpublisherForeignen_US
dc.publisherAmerican Chemical Societyen_US
dc.subjectSolvation Dynamicsen_US
dc.subjectLyotropic Liquiden_US
dc.subjectCrystalline Systemen_US
dc.subjectGood agreement with the measured diffusionen_US
dc.subject2015en_US
dc.titleSolvation Dynamics in Different Phases of the Lyotropic Liquid Crystalline Systemen_US
dc.typeArticleen_US

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