2012
DOI: 10.1007/s10884-012-9278-x
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Poisson–Nernst–Planck Systems for Ion Flow with Density Functional Theory for Hard-Sphere Potential: I–V Relations and Critical Potentials. Part II: Numerics

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Cited by 52 publications
(37 citation statements)
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“…This is the final result for the shape of the Coulomb staircase of occupancy as a function of Q f . Figure 2(b) shows qualitative agreement of P Q ( ) f shapes with (13), including the concentration-dependent shift between curves with different P b . We will make a more detailed comparison below.…”
Section: Shapes Of the Coulomb Blockade Oscillationsmentioning
confidence: 57%
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“…This is the final result for the shape of the Coulomb staircase of occupancy as a function of Q f . Figure 2(b) shows qualitative agreement of P Q ( ) f shapes with (13), including the concentration-dependent shift between curves with different P b . We will make a more detailed comparison below.…”
Section: Shapes Of the Coulomb Blockade Oscillationsmentioning
confidence: 57%
“…Ions in solution are surrounded by hydration shells with associated dehydration potential barriers that are also crucial for selectivity in many cases [5][6][7][8][9]. Selectivity frequently involves a 'knock on' mechanism or, more generally, the correlated motion of several ions [10][11][12][13]. The protein residues forming the 'locus' of the selectivity filter are amino acids, of which aspartate (D) and glutamate (E) have negatively charged side chains (Q e 1 f = − where e is the proton charge), lysine (K) has a positively charged side chain (Q e 1 f =+ ), and alanine (A) has a neutral side chain.…”
Section: Introductionmentioning
confidence: 99%
“…Without permanent charges, the flux of one ion species is independent of the other based on the classical PNP models for dilute mixtures (as is well known); for PNP with hard-sphere potentials, the flux of one ion species does depend on the other in the first order of characteristic ionic radius (see, e.g., [27,34,38]) due to ion-to-ion interactions. In this case, for both classical PNP and PNP with hard-sphere potentials studied in the abovementioned papers, only the average quantity H(1) of the channel geometry affects the fluxes.…”
Section: 3mentioning
confidence: 92%
“…A strategy for analyzing this connecting problem of classical PNP models was developed in [14] (in [36] for a general setting), which has been successfully extended to handle PNP with hard-sphere ions in [27,34,38]. The classical PNP system is first reduced to two subsystems: the limiting fast and the limiting slow system.…”
Section: Geometric Singular Perturbation Theory For (21)-(22)mentioning
confidence: 99%
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