Zobrazit minimální záznam

dc.contributor.authorBatko, Kornelia M.
dc.contributor.authorŚlęzak-Prochazka, Izabella
dc.contributor.authorŚlęzak, Andrzej
dc.contributor.authorBajdur, Wioletta M.
dc.contributor.authorŠčurek, Radomír
dc.date.accessioned2022-05-31T13:52:23Z
dc.date.available2022-05-31T13:52:23Z
dc.date.issued2022
dc.identifier.citationEntropy. 2022, vol. 24, issue 1, art. no. 138.cs
dc.identifier.issn1099-4300
dc.identifier.urihttp://hdl.handle.net/10084/146233
dc.description.abstractBased on Kedem-Katchalsky formalism, the model equation of the membrane potential (& UDelta;psi s) generated in a membrane system was derived for the conditions of concentration polarization. In this system, a horizontally oriented electro-neutral biomembrane separates solutions of the same electrolytes at different concentrations. The consequence of concentration polarization is the creation, on both sides of the membrane, of concentration boundary layers. The basic equation of this model includes the unknown ratio of solution concentrations (C-i/C-e) at the membrane/concentration boundary layers. We present the calculation procedure (C-i/C-e) based on novel equations derived in the paper containing the transport parameters of the membrane (L-p, sigma, and omega), solutions (rho, nu), concentration boundary layer thicknesses (delta(l), delta(h)), concentration Raileigh number (R-C), concentration polarization factor (zeta(s)), volume flux (J(v)), mechanical pressure difference (& UDelta;P), and ratio of known solution concentrations (C-h/C-l). From the resulting equation, & UDelta;psi(s) was calculated for various combinations of the solution concentration ratio (C-h/C-l), the Rayleigh concentration number (R-C), the concentration polarization coefficient (zeta(s)), and the hydrostatic pressure difference (& UDelta;P). Calculations were performed for a case where an aqueous NaCl solution with a fixed concentration of 1 mol m(-3) (C-l) was on one side of the membrane and on the other side an aqueous NaCl solution with a concentration between 1 and 15 mol m(-3) (C-h). It is shown that (& UDelta;psi(s)) depends on the value of one of the factors (i.e., & UDelta;P, C-h/C-l, R-C and zeta(s)) at a fixed value of the other three.cs
dc.language.isoencs
dc.publisherMDPIcs
dc.relation.ispartofseriesEntropycs
dc.relation.urihttps://doi.org/10.3390/e24010138cs
dc.rights© 2022 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.cs
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/cs
dc.subjectmembrane transportcs
dc.subjectmembrane potentialcs
dc.subjectconcentration polarizationcs
dc.subjectKedem–Katchalsky equationscs
dc.subjectpolymeric membranecs
dc.subjectconcentration Rayleigh numbercs
dc.titleModelling of the electrical membrane potential for concentration polarization conditionscs
dc.typearticlecs
dc.identifier.doi10.3390/e24010138
dc.rights.accessopenAccesscs
dc.type.versionpublishedVersioncs
dc.type.statusPeer-reviewedcs
dc.description.sourceWeb of Sciencecs
dc.description.volume24cs
dc.description.issue1cs
dc.description.firstpageart. no. 138cs
dc.identifier.wos000748434000001


Soubory tohoto záznamu

Tento záznam se objevuje v následujících kolekcích

Zobrazit minimální záznam

© 2022 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.
Kromě případů, kde je uvedeno jinak, licence tohoto záznamu je © 2022 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.