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Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study
The presence of a surface preferably attracting one component of a polymer mixture by the long-range van der Waals surface potential while the mixture undergoes phase separation by spinodal decomposition is called long-range surface-directed spinodal decomposition (SDSD). The morphology achieved und...
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/PMC7828815/ https://www.ncbi.nlm.nih.gov/pubmed/33466703 http://dx.doi.org/10.3390/polym13020256 |
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author | Ghaffari, Shima Chan, Philip K. Mehrvar, Mehrab |
author_facet | Ghaffari, Shima Chan, Philip K. Mehrvar, Mehrab |
author_sort | Ghaffari, Shima |
collection | PubMed |
description | The presence of a surface preferably attracting one component of a polymer mixture by the long-range van der Waals surface potential while the mixture undergoes phase separation by spinodal decomposition is called long-range surface-directed spinodal decomposition (SDSD). The morphology achieved under SDSD is an enrichment layer(s) close to the wall surface and a droplet-type structure in the bulk. In the current study of the long-range surface-directed polymerization-induced phase separation, the surface-directed spinodal decomposition of a monomer–solvent mixture undergoing self-condensation polymerization was theoretically simulated. The nonlinear Cahn–Hilliard and Flory–Huggins free energy theories were applied to investigate the phase separation phenomenon. The long-range surface potential led to the formation of a wetting layer on the surface. The thickness of the wetting layer was found proportional to time t*(1/5) and surface potential parameter h(1)(1/5). A larger diffusion coefficient led to the formation of smaller droplets in the bulk and a thinner depletion layer, while it did not affect the thickness of the enrichment layer close to the wall. A temperature gradient imposed in the same direction of long-range surface potential led to the formation of a stripe morphology near the wall, while imposing it in the opposite direction of surface potential led to the formation of large particles at the high-temperature side, the opposite side of the interacting wall. |
format | Online Article Text |
id | pubmed-7828815 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-78288152021-01-25 Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study Ghaffari, Shima Chan, Philip K. Mehrvar, Mehrab Polymers (Basel) Article The presence of a surface preferably attracting one component of a polymer mixture by the long-range van der Waals surface potential while the mixture undergoes phase separation by spinodal decomposition is called long-range surface-directed spinodal decomposition (SDSD). The morphology achieved under SDSD is an enrichment layer(s) close to the wall surface and a droplet-type structure in the bulk. In the current study of the long-range surface-directed polymerization-induced phase separation, the surface-directed spinodal decomposition of a monomer–solvent mixture undergoing self-condensation polymerization was theoretically simulated. The nonlinear Cahn–Hilliard and Flory–Huggins free energy theories were applied to investigate the phase separation phenomenon. The long-range surface potential led to the formation of a wetting layer on the surface. The thickness of the wetting layer was found proportional to time t*(1/5) and surface potential parameter h(1)(1/5). A larger diffusion coefficient led to the formation of smaller droplets in the bulk and a thinner depletion layer, while it did not affect the thickness of the enrichment layer close to the wall. A temperature gradient imposed in the same direction of long-range surface potential led to the formation of a stripe morphology near the wall, while imposing it in the opposite direction of surface potential led to the formation of large particles at the high-temperature side, the opposite side of the interacting wall. MDPI 2021-01-14 /pmc/articles/PMC7828815/ /pubmed/33466703 http://dx.doi.org/10.3390/polym13020256 Text en © 2021 by the authors. 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 (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Ghaffari, Shima Chan, Philip K. Mehrvar, Mehrab Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study |
title | Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study |
title_full | Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study |
title_fullStr | Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study |
title_full_unstemmed | Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study |
title_short | Long-Range Surface-Directed Polymerization-Induced Phase Separation: A Computational Study |
title_sort | long-range surface-directed polymerization-induced phase separation: a computational study |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7828815/ https://www.ncbi.nlm.nih.gov/pubmed/33466703 http://dx.doi.org/10.3390/polym13020256 |
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