1996
DOI: 10.1016/s0006-3495(96)79374-8
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Boundary conditions for- single-ion diffusion

Abstract: We have constructed a theory for diffusion through the pore of a single-ion channel by taking a limit of a random walk around a cycle of states. Similar to Levitt's theory of single-ion diffusion, one obtains boundary conditions for the Nernst-Planck equation that guarantee that the pore is occupied by at most one ion. Two of the terms in the boundary conditions are identical to those given by Levitt. However, the construction gives rise to a third term not found in Levitt's theory. With this term, the channel… Show more

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Cited by 42 publications
(58 citation statements)
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“…Framework models have been constructed to describe the permeation of single Na + ions (16) and single protons (2) through gramicidin. These models describe the dynamics of permeation in simplified configuration spaces that are designed to incorporate potentials of mean force and diffusion coefficients calculated by the molecular dynamics simulations.…”
Section: Summary and Discussionmentioning
confidence: 99%
See 2 more Smart Citations
“…Framework models have been constructed to describe the permeation of single Na + ions (16) and single protons (2) through gramicidin. These models describe the dynamics of permeation in simplified configuration spaces that are designed to incorporate potentials of mean force and diffusion coefficients calculated by the molecular dynamics simulations.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…The exponential distribution also underlies rate theory models (for example, ref. 18) and is an appropriate approximation when the concentration of excess protons in the surrounding baths is not too large (16,19). The boundary regions of the defect segment are modeled as the lumped states b I and b II .…”
Section: Lumped State Approximation Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…The stochastic Brownian motion of the multiion system was implemented as a continuous-time Markov chain with discrete states corresponding to the ion positions, and the state-to-state random walk was constructed by generating exponentially distributed random survival times. Such a Markov random walk satisfies the condition of detailed balance under equilibrium conditions in the absence of net flux, and the stochastic evolution of the system obeys a multidimensional Smulochowsky (Nernst-Planck) diffusion equation as ␦Z becomes increasingly small (30)(31)(32). The forward and backward transition rates are given by (e.g., for ion 1)…”
Section: Theory and Methodsmentioning
confidence: 99%
“…However, ion permeation is traditionally discussed in terms of the free-energy profile of ions along the channel axis (Hille, 2001). In particular, such quantity is an essential input to simple kinetic rate models (Läuger, 1973) and in the 1D Nernst-Planck (1D-NP) electrodiffusion equation (Levitt, 1986 ;McGill & Schumaker, 1996). From a dynamical point of view, the reduction in dimensionality from r to z is based on the assumption that all motions perpendicular to z reach equilibrium rapidly and that z is the only relevant slow variable in the system, i.e.…”
Section: Reduction To a One-dimensional (1d) Free-energy Profilementioning
confidence: 99%