Polymer–Surfactant Driven Interactions and the Resultant Microstructure in Protein-Containing Liquid Crystal Droplets

Integration of molecular liquid crystals (LCs) with functional proteins can provide new class of materials for potential applications in optical biosensing. However, hydrophobic nematic LCs (length ∼ 1–2 nm) and hydrophilic proteins, size ∼ O (nm), do not intermix without chemical modification of at...

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Published in:Langmuir Vol. 37; no. 41; pp. 11949 - 11960
Main Authors: Naveenkumar, Parinamipura M, Singh, Raju Kumar, Mann, Stephen, Seth, Jyoti R, Sharma, Kamendra P
Format: Journal Article
Language:English
Published: American Chemical Society 19-10-2021
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Summary:Integration of molecular liquid crystals (LCs) with functional proteins can provide new class of materials for potential applications in optical biosensing. However, hydrophobic nematic LCs (length ∼ 1–2 nm) and hydrophilic proteins, size ∼ O (nm), do not intermix without chemical modification of at least one of them. Bioconjugation of proteins with a polyethylene glycol-based polymeric surfactant (PS) can provide a core–shell system that is sequestered within nonaqueous LC (4-cyano-4′-pentylbiphenyl) microdroplets. However, the nature of interactions between the components and detailed understanding of the resultant hybrid microstructure remains unclear. Here, using a combination of isothermal titration calorimetry (ITC), fluorescence microscopy, and infrared-imaging spectroscopy, we show that strong hydrophobic interactions between the LC and PS drives the sequestration of a myoglobin–PS (Mb–PS; dispersed in the aqueous phase) into the LC spherical microdroplets or even into a bulk LC phase. The average values of both, the binding constant and the standard molar enthalpy change, are increased by approximately a factor of 2.5 times when the unmodified Mb is conjugated to the PS. Small-angle X-ray scattering studies reveal that LC molecules act as a solvent for the Mb–PS conjugate; furthermore, the LC long-range order is disturbed due to mixing, as exemplified by the change in its coherence length from 8.9 to 5.7 nm. Detailed all-atomistic molecular dynamic simulations for a three-component PS–water–LC system show a change in interaction energy of −144 kJ mol–1 PS–1 upon the contact of PS chains (initially dispersed in water) with LC and agree with the ITC experiments.
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ISSN:0743-7463
1520-5827
DOI:10.1021/acs.langmuir.1c00960