| نویسندگان | Fatemeh Ebrahimi,Mehdi Neek-Amal,Muhammad Sahimi |
| نشریه | Journal of Physical Chemistry B |
| شماره صفحات | 10727-10734 |
| شماره سریال | 43 |
| شماره مجلد | 128 |
| ضریب تاثیر (IF) | 3.377 |
| نوع مقاله | Full Paper |
| تاریخ انتشار | 2024 |
| نوع نشریه | چاپی |
| کشور محل چاپ | ایران |
| نمایه نشریه | ISI،JCR،Scopus |
چکیده مقاله
Taylor−Aris (T−A) dispersion of a solute in a flowing solvent is a fundamental phenomenon in most mass-transfer
processes. Despite its significance and numerous applications in microreactors, colloidal transport in confined media,
chromatographic separation, and transport in biological tissues, the effect of the slip length and the topology of surface potential
landscapes on T−A dispersion in nanostructured channels has not been studied in detail. We propose a novel methodology for
molecular dynamics (MD) simulation of T−A dispersion in such systems, derive an analytical expression for the dispersion
coefficient in them, and report on the results of extensive MD simulations of the phenomenon in carbon nanotubes and hexagonal
carbon nanochannels. By broadening the topology of the surface energy landscape, we vary the slip lengths, making it possible to
distinguish between the effects of confinement, the topology of the energy landscape, and the slip length on the T−A dispersion
coefficient. It is demonstrated that measuring the T−A dispersion coefficient in laminar flow is a straightforward and reliable
approach for estimating the slip length in nanotubes and other nanostructured materials.
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