charged polymer
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2021 ◽  
Author(s):  
Kaushik Chakraborty ◽  
Prabir Khatua ◽  
Wataru Shinoda ◽  
Sharon M. Loverde

Polymers ◽  
2021 ◽  
Vol 13 (16) ◽  
pp. 2800
Author(s):  
Christopher Hill ◽  
Wasiu Abdullahi ◽  
Robert Dalgliesh ◽  
Martin Crossman ◽  
Peter Charles Griffiths

Oppositely charged polymer–surfactant complexes are frequently explored as a function of phase space defined by the charge ratio Z, (where Z = [+polymer]/[−surfactant]), 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 [+polymer] at fixed Cpolymer. The nanostructures were characterised by small-angle neutron scattering (SANS) in D2O 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 (CSDS < 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.


2021 ◽  
Vol 111 ◽  
pp. 103577
Author(s):  
Albraa A. Jaber ◽  
Ahmad Abu Obaid ◽  
Suresh G. Advani ◽  
John W. Gillespie

2021 ◽  
Author(s):  
Douglas J. Grzetic ◽  
Kris T. Delaney ◽  
Glenn H. Fredrickson

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