2022
DOI: 10.1007/s00396-022-05007-8
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Ion partitioning and ion size effects on streaming field and energy conversion efficiency in a soft nanochannel

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Cited by 7 publications
(11 citation statements)
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“…The augment of efficiency can be an order increase compared to the ion-partitioning effects not being considered, with a maximum of ∼12% efficiency presented [169]. A recent study by Kundu et al draws similar conclusions that the streaming potential and energy conversion efficiency amplify when the ion partitioning effect becomes significant [170] in the case of high surface charge density or thick PEL [171].…”
Section: Classical Nanofluidics Ekecmentioning
confidence: 77%
See 1 more Smart Citation
“…The augment of efficiency can be an order increase compared to the ion-partitioning effects not being considered, with a maximum of ∼12% efficiency presented [169]. A recent study by Kundu et al draws similar conclusions that the streaming potential and energy conversion efficiency amplify when the ion partitioning effect becomes significant [170] in the case of high surface charge density or thick PEL [171].…”
Section: Classical Nanofluidics Ekecmentioning
confidence: 77%
“…A recent study by Kundu et al. draws similar conclusions that the streaming potential and energy conversion efficiency amplify when the ion partitioning effect becomes significant [170] in the case of high surface charge density or thick PEL [171].…”
Section: Performance Of Energy Conversionmentioning
confidence: 87%
“…The boundary conditions associated with coupled eqs – are as follows: The electric potential is taken as ϕ(cis) = 0 and ϕ(trans) = V 0 . The ionic concentration at the ends of the reservoir is maintained at bulk values, c i = c 0 . The rigid surface of the membrane is ion-impenetrable with flux n · N i = 0 and uncharged − n ·∇ϕ = 0. The surface of the DNA nanoparticle has a convective flux of n · N i = n ·( u c i ) due to an ion-impenetrable surface and also has a constant surface charge density of − n ·∇ϕ = σ p /ε f = λ DNA /(2 πaε f ), where λ DNA = λ bare /β M is the effective line charge density with the bare line charge density of DNA, λ bare = 5.9 e nm –1 , and the Manning factor, β M = 4.2 A normal flow with p = 0 is applied at both ends of the compartment. The no-slip condition is assumed for both the surface of DNA and the membrane, giving u = U p e z , and u = 0, respectively, where U p is the electrophoretic velocity of the DNA obtained from balancing the z component of the electric force, F E , and the hydrodynamic force, F H . The electric potential, the electric field, and the flow field are continuous at the PEL–liquid interface. The ionic concentration at the PEL–liquid interface is discontinuous. c P E L c f = exp ( Δ W i k B T ) c PEL and c f are the ionic concentrations in PEL and the bulk fluid domain, respectively, k B is the Boltzmann constant, and Δ W i is the energy difference of the i th ionic species given as ,, normalΔ W i = false( z i e false) 2 8 π r i ( 1 ε P E L…”
Section: Modelingmentioning
confidence: 99%
“…Note that the gradual variation of monomers as well as charge distribution is controlled via decay length, which further recovers the uniform distribution of both of these quantities at the vanishing limit of decay length. Later, several researchers studied the electrophoresis of diffuse polymeric layer coated composite structured nanoparticles 81,82 as well as electrokinetic flow through nanopores where the walls are coated with a diffuse polymer layer, 83,84 considering the structural charge within a polymer layer as independent of bulk pH. Note that there is no available literature which deals with the electrophoresis of diffuse porous particles comprised of pH-regulated structural charge and considering the impact of the ion steric effect.…”
Section: Introductionmentioning
confidence: 99%