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Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles
Aqueous solutions of a nonionic surfactant (either Tween20 or BrijL23) and an anionic surfactant (sodium dodecyl sulfate, SDS) are investigated, using small-angle neutron scattering (SANS). SANS spectra are analysed by using a core-shell model to describe the form factor of self-assembled surfactant...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8307929/ https://www.ncbi.nlm.nih.gov/pubmed/34299413 http://dx.doi.org/10.3390/molecules26144136 |
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author | Ludwig, Michael Geisler, Ramsia Prévost, Sylvain von Klitzing, Regine |
author_facet | Ludwig, Michael Geisler, Ramsia Prévost, Sylvain von Klitzing, Regine |
author_sort | Ludwig, Michael |
collection | PubMed |
description | Aqueous solutions of a nonionic surfactant (either Tween20 or BrijL23) and an anionic surfactant (sodium dodecyl sulfate, SDS) are investigated, using small-angle neutron scattering (SANS). SANS spectra are analysed by using a core-shell model to describe the form factor of self-assembled surfactant micelles; the intermicellar interactions are modelled by using a hard-sphere Percus–Yevick (HS-PY) or a rescaled mean spherical approximation (RMSA) structure factor. Choosing these specific nonionic surfactants allows for comparison of the effect of branched (Tween20) and linear (BrijL23) surfactant headgroups, both constituted of poly-ethylene oxide (PEO) groups. The nonionic–anionic surfactant mixtures are studied at various concentrations up to highly concentrated samples ([Formula: see text] ≲ 0.45) and various mixing ratios, from pure nonionic to pure anionic surfactant solutions. The scattering data reveal the formation of mixed micelles already at concentrations below the critical micelle concentration of SDS. At higher volume fractions, excluded volume effects dominate the intermicellar structuring, even for charged micelles. In consequence, at high volume fractions, the intermicellar structuring is the same for charged and uncharged micelles. At all mixing ratios, almost spherical mixed micelles form. This offers the opportunity to create a system of colloidal particles with a variable surface charge. This excludes only roughly equimolar mixing ratios (X≈ 0.4–0.6) at which the micelles significantly increase in size and ellipticity due to specific sulfate–EO interactions. |
format | Online Article Text |
id | pubmed-8307929 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-83079292021-07-25 Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles Ludwig, Michael Geisler, Ramsia Prévost, Sylvain von Klitzing, Regine Molecules Article Aqueous solutions of a nonionic surfactant (either Tween20 or BrijL23) and an anionic surfactant (sodium dodecyl sulfate, SDS) are investigated, using small-angle neutron scattering (SANS). SANS spectra are analysed by using a core-shell model to describe the form factor of self-assembled surfactant micelles; the intermicellar interactions are modelled by using a hard-sphere Percus–Yevick (HS-PY) or a rescaled mean spherical approximation (RMSA) structure factor. Choosing these specific nonionic surfactants allows for comparison of the effect of branched (Tween20) and linear (BrijL23) surfactant headgroups, both constituted of poly-ethylene oxide (PEO) groups. The nonionic–anionic surfactant mixtures are studied at various concentrations up to highly concentrated samples ([Formula: see text] ≲ 0.45) and various mixing ratios, from pure nonionic to pure anionic surfactant solutions. The scattering data reveal the formation of mixed micelles already at concentrations below the critical micelle concentration of SDS. At higher volume fractions, excluded volume effects dominate the intermicellar structuring, even for charged micelles. In consequence, at high volume fractions, the intermicellar structuring is the same for charged and uncharged micelles. At all mixing ratios, almost spherical mixed micelles form. This offers the opportunity to create a system of colloidal particles with a variable surface charge. This excludes only roughly equimolar mixing ratios (X≈ 0.4–0.6) at which the micelles significantly increase in size and ellipticity due to specific sulfate–EO interactions. MDPI 2021-07-07 /pmc/articles/PMC8307929/ /pubmed/34299413 http://dx.doi.org/10.3390/molecules26144136 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Ludwig, Michael Geisler, Ramsia Prévost, Sylvain von Klitzing, Regine Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles |
title | Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles |
title_full | Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles |
title_fullStr | Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles |
title_full_unstemmed | Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles |
title_short | Shape and Structure Formation of Mixed Nonionic–Anionic Surfactant Micelles |
title_sort | shape and structure formation of mixed nonionic–anionic surfactant micelles |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8307929/ https://www.ncbi.nlm.nih.gov/pubmed/34299413 http://dx.doi.org/10.3390/molecules26144136 |
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