2018
DOI: 10.1016/j.memsci.2017.11.073
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On the origin of membrane potential in membranes with polarizable nanopores

Abstract: We report a new mechanism for the generation of membrane potential in polarizable nanoporous membranes separating electrolytes with different concentrations. The electric field generated by diffusion of ions with different mobilities induces a non-uniform surface charge, which results in charge separation inside the nanopore. The corresponding Donnan potentials appear at the pore entrance and exit leading to a dramatic enhancement of membrane potential in comparison with an uncharged non-polarizable membrane. … Show more

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Cited by 33 publications
(41 citation statements)
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“…[12] The SC model is centred on the combination of the Navier-Stokes, Poisson and Nernst-Planck equations and can be derived to account for immobile or ionizible charges and fluid slip on the pore walls . [13,14,15,16,17,18,19,20,21] The UP model drops the radial dependence of the electrical potential in the pore as described by the Poisson equation and consider the radial potential uniform. [22,23,24,25,26] This simplification limits the validity of the UP model to dilute solutions and narrow pore diameters; This condition is fulfilled when the electrical double layers (EDLs) inside the pores overlap.…”
Section: Introductionmentioning
confidence: 99%
“…[12] The SC model is centred on the combination of the Navier-Stokes, Poisson and Nernst-Planck equations and can be derived to account for immobile or ionizible charges and fluid slip on the pore walls . [13,14,15,16,17,18,19,20,21] The UP model drops the radial dependence of the electrical potential in the pore as described by the Poisson equation and consider the radial potential uniform. [22,23,24,25,26] This simplification limits the validity of the UP model to dilute solutions and narrow pore diameters; This condition is fulfilled when the electrical double layers (EDLs) inside the pores overlap.…”
Section: Introductionmentioning
confidence: 99%
“…When the membrane is not charged externally by injecting or withdrawing electrons to or from the conductive membrane pore walls, one has X e = 0. However, even then the local value X e (z) can be non-zero since electrons are redistributed along the surface in order to ensure equipotential in the pore wall [33,44]. The volumetric density of wall charge is X = X c + X e , which is opposite in sign to the density of ionic charges c + − c − in the pore because of total charge neutrality…”
Section: Theoretical Modelmentioning
confidence: 99%
“…Therefore, it is necessary to control the transport and selective properties of a membrane in order to preserve it from any influence caused by these limitations. There are two main ways to affect the membrane's selective properties: changing the structure of pores (the geometry and physico-chemical properties of the surface) [10,11], including using composite membranes [12]) or external exposure (transmembrane potential, external electric fields [13][14][15], pH of the solution [16], temperature, radiation, etc. ).…”
Section: Introductionmentioning
confidence: 99%
“…However, this method is difficult to use, for example, in the synthesis of inorganic solid membranes. The surface modification technique is the most convenient method in this case [11]. The surface modification technique deals with deposition of nanoparticles onto a membrane.Silicate (high silica) porous glasses (PGs) are channel-type nanostructures [20] with thermal, chemical and microbiological stability, in combination with controlled surface structural characteristics [21][22][23].…”
mentioning
confidence: 99%
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