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Charge Modification as a Mechanism for Tunable Properties in Polymer–Surfactant Complexes

Oppositely charged polymer–surfactant complexes are frequently explored as a function of phase space defined by the charge ratio Z, (where Z = [[Formula: see text]), commonly accessed through the surfactant concentration. Tuning the phase behaviour and related properties of these complexes is an imp...

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Detalles Bibliográficos
Autores principales: Hill, Christopher, Abdullahi, Wasiu, Dalgliesh, Robert, Crossman, Martin, Griffiths, Peter Charles
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8397960/
https://www.ncbi.nlm.nih.gov/pubmed/34451340
http://dx.doi.org/10.3390/polym13162800
Descripción
Sumario:Oppositely charged polymer–surfactant complexes are frequently explored as a function of phase space defined by the charge ratio Z, (where Z = [[Formula: see text]), commonly accessed through the surfactant concentration. Tuning the phase behaviour and related properties of these complexes is an important tool for optimising commercial formulations; hence, understanding the relationship between Z and bulk properties is pertinent. Here, within a homologous series of cationic hydroxyethyl cellulose (cat-HEC) polymers with minor perturbations in the degree of side chain charge modification, phase space is instead explored through [Formula: see text] at fixed C [Formula: see text]. The nanostructures were characterised by small-angle neutron scattering (SANS) in D [Formula: see text] O solutions and in combination with the oppositely charged surfactant sodium dodecylsulfate (h- or d-SDS). Scattering consistent with thin rods with an average radius of ∼7.7 Å and length of ∼85 Å was observed for all cat-HEC polymers and no significant interactions were shown between the neutral HEC polymer and SDS (C [Formula: see text] < CMC). For the charge-modified polymers, interactions with SDS were evident and the radius of the formed complexes grew up to ∼15 Å with increasing Z. This study demonstrates a novel approach in which the Z phase space of oppositely charged polymer–surfactant complexes can be controlled at fixed concentrations.